Optical Image Capturing System

ABSTRACT

A six-piece optical lens for capturing image and a six-piece optical module for capturing image are provided. In order from an object side to an image side, the optical lens along the optical axis includes a first lens with refractive power, a second lens with refractive power, a third lens with refractive power, a fourth lens with refractive power, a fifth lens with refractive power and a sixth lens with refractive power. At least one of the image-side surface and object-side surface of each of the six lens elements is aspheric. The optical lens can increase aperture value and improve the imagining quality for use in compact cameras.

CROSS-REFERENCE TO RELATED APPLICATION

This application claims the benefit of Taiwan Patent Application No.104140608, filed on Dec. 3, 2015, in the Taiwan Intellectual PropertyOffice, the disclosure of which is incorporated herein in its entiretyby reference.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present disclosure relates to an optical image capturing system, andmore particularly to a compact optical image capturing system which canbe applied to electronic products.

2. Description of the Related Art

In recent years, with the rise of portable electronic devices havingcamera functionalities, the demand for an optical image capturing systemis raised gradually. The image sensing device of ordinary photographingcamera is commonly selected from charge coupled device (CCD) orcomplementary metal-oxide semiconductor sensor (CMOS Sensor). Inaddition, as advanced semiconductor manufacturing technology enables theminimization of pixel size of the image sensing device, the developmentof the optical image capturing system directs towards the field of highpixels. Therefore, the requirement for high imaging quality is rapidlyraised.

The traditional optical image capturing system of a portable electronicdevice comes with different designs, including a four-lens or afive-lens design. However, the requirement for the higher pixels and therequirement for a large aperture of an end user, like functionalities ofmicro filming and night view, or the requirement of wide view angle ofthe portable electronic device have been raised. But the optical imagecapturing system with the large aperture design often produces moreaberration resulting in the deterioration of quality in peripheral imageformation and difficulties of manufacturing, and the optical imagecapturing system with wide view angle design increases distortion ratein image formation, thus the optical image capturing system in priorarts cannot meet the requirement of the higher order camera lens module.

Therefore, how to effectively increase quantity of incoming light andview angle of the optical lenses, not only further improves total pixelsand imaging quality for the image formation, but also considers theequity design of the miniaturized optical lenses, becomes a quiteimportant issue.

SUMMARY OF THE INVENTION

The aspect of embodiment of the present disclosure directs to an opticalimage capturing system and an optical image capturing lens which usecombination of refractive powers, convex and concave surfaces ofsix-piece optical lenses (the convex or concave surface in thedisclosure denotes the geometrical shape of an image-side surface or anobject-side surface of each lens on an optical axis) to increase thequantity of incoming light of the optical image capturing system and theview angle of the optical lenses, and to improve total pixels andimaging quality for image formation, so as to be applied to minimizedelectronic products.

The term and its definition to the lens element parameter in theembodiment of the present invention are shown as below for furtherreference.

The lens element parameter related to a length or a height in the lenselement

A maximum height for image formation of the optical image capturingsystem is denoted by HOI. A height of the optical image capturing systemis denoted by HOS. A distance from the object-side surface of the firstlens element to the image-side surface of the sixth lens element isdenoted by InTL. A distance from an aperture stop (aperture) to an imageplane is denoted by InS. A distance from the first lens element to thesecond lens element is denoted by In12 (instance). A central thicknessof the first lens element of the optical image capturing system on theoptical axis is denoted by TP1 (instance).

The lens element parameter related to a material in the lens element

An Abbe number of the first lens element in the optical image capturingsystem is denoted by NA1 (instance). A refractive index of the firstlens element is denoted by Nd1 (instance).

The lens element parameter related to a view angle in the lens element

A view angle is denoted by AF. Half of the view angle is denoted by HAF.A major light angle is denoted by MRA.

The lens element parameter related to exit/entrance pupil in the lenselement

An entrance pupil diameter of the optical image capturing system isdenoted by HEP. A maximum effective half diameter (EHD) of any surfaceof a single lens element refers to a perpendicular height between anintersection point on the surface of the lens element where the incidentlight with the maximum view angle in the optical system passes throughthe outmost edge of the entrance pupil and the optical axis. Forexample, the maximum effective half diameter of the object-side surfaceof the first lens element is denoted by EHD 11. The maximum effectivehalf diameter of the image-side surface of the first lens element isdenoted by EHD 12. The maximum effective half diameter of theobject-side surface of the second lens element is denoted by EHD 21. Themaximum effective half diameter of the image-side surface of the secondlens element is denoted by EHD 22. The maximum effective half diametersof any surfaces of other lens elements in the optical image capturingsystem are denoted in the similar way.

The lens element parameter related to a depth of the lens element shape

A distance in parallel with an optical axis from a maximum effectivediameter position to an axial point on the object-side surface of thesixth lens element is denoted by InRS61 (instance). A distance inparallel with an optical axis from a maximum effective diameter positionto an axial point on the image-side surface of the sixth lens element isdenoted by InRS62 (instance).

The lens element parameter related to the lens element shape

A critical point C is a tangent point on a surface of a specific lenselement, and the tangent point is tangent to a plane perpendicular tothe optical axis and the tangent point cannot be a crossover point onthe optical axis. To follow the past, a distance perpendicular to theoptical axis between a critical point C51 on the object-side surface ofthe fifth lens element and the optical axis is HVT51 (instance). Adistance perpendicular to the optical axis between a critical point C52on the image-side surface of the fifth lens element and the optical axisis HVT52 (instance). A distance perpendicular to the optical axisbetween a critical point C61 on the object-side surface of the sixthlens element and the optical axis is HVT61 (instance). A distanceperpendicular to the optical axis between a critical point C62 on theimage-side surface of the sixth lens element and the optical axis isHVT62 (instance). Distances perpendicular to the optical axis betweencritical points on the object-side surfaces or the image-side surfacesof other lens elements and the optical axis are denoted in the similarway described above.

The object-side surface of the sixth lens element has one inflectionpoint IF611 which is nearest to the optical axis, and the sinkage valueof the inflection point IF611 is denoted by SGI611 (instance). SGI611 isa horizontal shift distance in parallel with the optical axis from anaxial point on the object-side surface of the sixth lens element to theinflection point which is nearest to the optical axis on the object-sidesurface of the sixth lens element. A distance perpendicular to theoptical axis between the inflection point IF611 and the optical axis isHIF611 (instance). The image-side surface of the sixth lens element hasone inflection point IF621 which is nearest to the optical axis and thesinkage value of the inflection point IF621 is denoted by SGI621(instance). SGI621 is a horizontal shift distance in parallel with theoptical axis from an axial point on the image-side surface of the sixthlens element to the inflection point which is nearest to the opticalaxis on the image-side surface of the sixth lens element. A distanceperpendicular to the optical axis between the inflection point IF621 andthe optical axis is HIF621 (instance).

The object-side surface of the sixth lens element has one inflectionpoint IF612 which is the second nearest to the optical axis and thesinkage value of the inflection point IF612 is denoted by SGI612(instance). SGI612 is a horizontal shift distance in parallel with theoptical axis from an axial point on the object-side surface of the sixthlens element to the inflection point which is the second nearest to theoptical axis on the object-side surface of the sixth lens element. Adistance perpendicular to the optical axis between the inflection pointIF612 and the optical axis is HIF612 (instance). The image-side surfaceof the sixth lens element has one inflection point IF622 which is thesecond nearest to the optical axis and the sinkage value of theinflection point IF622 is denoted by SGI622 (instance). SGI622 is ahorizontal shift distance in parallel with the optical axis from anaxial point on the image-side surface of the sixth lens element to theinflection point which is the second nearest to the optical axis on theimage-side surface of the sixth lens element. A distance perpendicularto the optical axis between the inflection point IF622 and the opticalaxis is HIF622 (instance).

The object-side surface of the sixth lens element has one inflectionpoint IF613 which is the third nearest to the optical axis and thesinkage value of the inflection point IF613 is denoted by SGI613(instance). SGI613 is a horizontal shift distance in parallel with theoptical axis from an axial point on the object-side surface of the sixthlens element to the inflection point which is the third nearest to theoptical axis on the object-side surface of the sixth lens element. Adistance perpendicular to the optical axis between the inflection pointIF613 and the optical axis is HIF613 (instance). The image-side surfaceof the sixth lens element has one inflection point IF623 which is thethird nearest to the optical axis and the sinkage value of theinflection point IF623 is denoted by SGI623 (instance). SGI623 is ahorizontal shift distance in parallel with the optical axis from anaxial point on the image-side surface of the sixth lens element to theinflection point which is the third nearest to the optical axis on theimage-side surface of the sixth lens element. A distance perpendicularto the optical axis between the inflection point IF623 and the opticalaxis is HIF623 (instance).

The object-side surface of the sixth lens element has one inflectionpoint IF614 which is the fourth nearest to the optical axis and thesinkage value of the inflection point IF614 is denoted by SGI614(instance). SGI614 is a horizontal shift distance in parallel with theoptical axis from an axial point on the object-side surface of the sixthlens element to the inflection point which is the fourth nearest to theoptical axis on the object-side surface of the sixth lens element. Adistance perpendicular to the optical axis between the inflection pointIF614 and the optical axis is HIF614 (instance). The image-side surfaceof the sixth lens element has one inflection point IF624 which is thefourth nearest to the optical axis and the sinkage value of theinflection point IF624 is denoted by SGI624 (instance). SGI624 is ahorizontal shift distance in parallel with the optical axis from anaxial point on the image-side surface of the sixth lens element to theinflection point which is the fourth nearest to the optical axis on theimage-side surface of the sixth lens element. A distance perpendicularto the optical axis between the inflection point IF624 and the opticalaxis is HIF624 (instance).

The inflection points on the object-side surfaces or the image-sidesurfaces of the other lens elements and the distances perpendicular tothe optical axis thereof or the sinkage values thereof are denoted inthe similar way described above.

The lens element parameter related to an aberration

Optical distortion for image formation in the optical image capturingsystem is denoted by ODT. TV distortion for image formation in theoptical image capturing system is denoted by TDT. Further, the range ofthe aberration offset for the view of image formation may be limited to50%-100%. An offset of the spherical aberration is denoted by DFS. Anoffset of the coma aberration is denoted by DFC.

The vertical coordinate axis of the characteristic diagram of modulationtransfer function represents a contrast transfer rate (values are from 0to 1). The horizontal coordinate axis represents a spatial frequency(cycles/mm; lp/mm; line pairs per mm). Theoretically, an ideal imagecapturing system can 100% show the line contrast of a photographedobject. However, the values of the contrast transfer rate at thevertical coordinate axis are smaller than 1 in the actual imagecapturing system. The transfer rate of its comparison value is less thana vertical axis. In addition, comparing to the central region, it isgenerally more difficult to achieve a fine degree of recovery in theedge region of image capturing. The contrast transfer rates (MTF values)with spatial frequencies of 55 cycles/m at the optical axis, 0.3 fieldof view and 0.7 field of view of a visible spectrum on the image planeare respectively denoted by MTFE0, MTFE3 and MTFE7. The contrasttransfer rates (MTF values) with spatial frequencies of 110 cycles/m atthe optical axis, 0.3 field of view and 0.7 field of view on the imageplane are respectively denoted by MTFQ0, MTFQ3 and MTFQ7. The contrasttransfer rates (MTF values) with spatial frequencies of 220 cycles/m atthe optical axis, 0.3 field of view and 0.7 field of view on the imageplane are respectively denoted by MTFH0, MTFH3 and MTFH7. The contrasttransfer rates (MTF values) with spatial frequencies of 440 cycles/m atthe optical axis, 0.3 field of view and 0.7 field of view on the imageplane are respectively denoted by MTF0, MTF3 and MTF7. The three fieldsof view described above are representative to the center, the internalfield of view and the external field of view of the lens elements. Thus,they may be used to evaluate whether the performance of a specificoptical image capturing system is excellent. The design of the opticalimage capturing system of the present invention mainly corresponds to apixel size in which a sensing device below 1.12 micrometers is includes.Therefore, the quarter spatial frequencies, the half spatial frequencies(half frequencies) and the full spatial frequencies (full frequencies)of the characteristic diagram of modulation transfer functionrespectively are at least 110 cycles/mm, 220 cycles/mm and 440cycles/mm.

If an optical image capturing system needs to satisfy with the imagesaimed to infrared spectrum, such as the requirement for night visionwith lower light source, the used wavelength may be 850 nm or 800 nm. Asthe main function is to recognize shape of an object formed inmonochrome and shade, the high resolution is unnecessary, and thus, aspatial frequency, which is less than 110 cycles/mm, is used to evaluatethe functionality of the optical image capturing system, when theoptical image capturing system is applied to the infrared spectrum. Whenthe foregoing wavelength 850 nm is applied to focus on the image plane,the contrast transfer rates (MTF values) with a spatial frequency of 55cycles/mm at the optical axis, 0.3 field of view and 0.7 field of viewon the image plane are respectively denoted by MTFI0, MTFI3 and MTFI7.However, the infrared wavelength of 850 nm or 800 nm may be hugelydifferent to wavelength of the regular visible light wavelength, andthus, it is hard to design an optical image capturing system which hasto focus on the visible light and the infrared light (dual-mode)simultaneously while achieve a certain function respectively.

The disclosure provides an optical image capturing system, which is ableto focus on the visible light and the infrared light (dual-mode)simultaneously while achieve a certain function respectively, and anobject-side surface or an image-side surface of the fourth lens elementhas inflection points, such that the angle of incidence from each fieldof view to the fourth lens element can be adjusted effectively and theoptical distortion and the TV distortion can be corrected as well.Besides, the surfaces of the fourth lens element may have a betteroptical path adjusting ability to acquire better imaging quality.

The disclosure provides an optical image capturing system, in order froman object side to an image side, including a first, second, third,fourth, fifth, sixth lens elements and an image plane. The first lenselement has refractive power. Focal lengths of the first through sixthlens elements are f1, f2, f3, f4, f5 and f6 respectively. A focal lengthof the optical image capturing system is f. An entrance pupil diameterof the optical image capturing system is HEP. A distance from anobject-side surface of the first lens element to the image plane is HOS.A half of a maximum view angle of the optical image capturing system isHAF. Thicknesses in parallel with an optical axis of the first throughsixth lens elements at height ½ HEP respectively are ETP1, ETP2, ETP3,ETP4, ETP5 and ETP6. A sum of ETP1 to ETP6 described above is SETP.Thicknesses of the first through sixth lens elements on the optical axisrespectively are TP1, TP2, TP3, TP4, TP5 and TP6. A sum of TP1 to TP6described above is STP. The following relations are satisfied:1.0≦f/HEP≦10.0, 0 deg<HAF≦150 deg and 0.5≦SETP/STP<1.

The disclosure provides another optical image capturing system, in orderfrom an object side to an image side, including a first, second, third,fourth, fifth, sixth lens elements and an image plane. The first lenselement has refractive power. The second lens element has refractivepower. The third lens element has refractive power. The fourth lenselement has refractive power. The fifth lens element has refractivepower. The sixth lens element has refractive power. At least two lenselements among the first through sixth lens element have at least oneinflection point on at least one surface thereof. At least one lenselement among the first through third lens elements has positiverefractive power, and at least one lens element among the fourth throughsixth lens elements has positive refractive power. A focal length of theoptical image capturing system is f. Focal lengths of the first throughsixth lens elements are f1, f2, f3, f4, f5 and f6 respectively. Anentrance pupil diameter of the optical image capturing system is HEP. Adistance from an object-side surface of the first lens element to theimage plane is HOS. A half of a maximum view angle of the optical imagecapturing system is HAF. A horizontal distance in parallel with theoptical axis from a coordinate point on the object-side surface of thefirst lens element at height ½ HEP to the image plane is ETL. Ahorizontal distance in parallel with the optical axis from a coordinatepoint on the object-side surface of the first lens element at height ½HEP to a coordinate point on the image-side surface of the sixth lenselement at height ½ HEP is EIN. The following relations are satisfied:1.0≦f/HEP≦10.0, 0 deg<HAF≦150 deg and 0.2≦EIN/ETL<1.

The disclosure provides another optical image capturing system, in orderfrom an object side to an image side, including a first, second, third,fourth, fifth, sixth lens elements and an image plane. Wherein theoptical image capturing system consists of six lens elements withrefractive power. The first lens element has positive refractive power.The second lens element has refractive power. The third lens element hasrefractive power. The fourth lens element has refractive power. Thefifth lens element has refractive power. The sixth lens element hasrefractive power. At least one lens element among the second throughsixth lens elements has positive refractive power. At least three lenselements among the first through sixth lens element respectively have atleast one inflection point on at least one surface thereof. Focallengths of the first through sixth lens elements are f1, f2, f3, f4, f5and f6 respectively. A focal length of the optical image capturingsystem is f. An entrance pupil diameter of the optical image capturingsystem is HEP. A distance from an object-side surface of the first lenselement to the image plane is HOS. A half of maximum view angle of theoptical image capturing system is HAF. A horizontal distance in parallelwith the optical axis from a coordinate point on the object-side surfaceof the first lens element at height ½ HEP to the image plane is ETL. Ahorizontal distance in parallel with the optical axis from a coordinatepoint on the object-side surface of the first lens element at height ½HEP to a coordinate point on the image-side surface of the sixth lenselement at height ½ HEP is EIN. The following relations are satisfied:1.0≦f/HEP≦3.5, 0 deg<HAF≦150 deg and 0.2≦EIN/ETL<1.

A thickness of a single lens element at height of ½ entrance pupildiameter (HEP) particularly affects the corrected aberration of commonarea of each field of view of light and the capability of correctingoptical path difference between each field of view of light in the scopeof ½ entrance pupil diameter (HEP). The capability of aberrationcorrection is enhanced if the thickness becomes greater, but thedifficulty for manufacturing is also increased at the same time.Therefore, it is necessary to control the thickness of a single lenselement at height of ½ entrance pupil diameter (HEP), in particular tocontrol the ratio relation (ETP/TP) of the thickness (ETP) of the lenselement at height of ½ entrance pupil diameter (HEP) to the thickness(TP) of the lens element to which the surface belongs on the opticalaxis. For example, the thickness of the first lens element at height of½ entrance pupil diameter (HEP) is denoted by ETP1. The thickness of thesecond lens element at height of ½ entrance pupil diameter (HEP) isdenoted by ETP2. The thicknesses of other lens elements are denoted inthe similar way. A sum of ETP1 to ETP6 described above is SETP. Theembodiments of the present invention may satisfy the following relation:0.3≦SETP/EIN<1.

In order to enhance the capability of aberration correction and reducethe difficulty for manufacturing at the same time, it is particularlynecessary to control the ratio relation (ETP/TP) of the thickness (ETP)of the lens element at height of ½ entrance pupil diameter (HEP) to thethickness (TP) of the lens element on the optical axis lens. Forexample, the thickness of the first lens element at height of ½ entrancepupil diameter (HEP) is denoted by ETP1. The thickness of the first lenselement on the optical axis is TP1. The ratio between both of them isETP1/TP1. The thickness of the second lens element at height of ½entrance pupil diameter (HEP) is denoted by ETP2. The thickness of thesecond lens element on the optical axis is TP2. The ratio between bothof them is ETP2/TP2. The ratio relations of the thicknesses of otherlens element in the optical image capturing system at height of ½entrance pupil diameter (HEP) to the thicknesses (TP) of the lenselements on the optical axis lens are denoted in the similar way. Theembodiments of the present invention may satisfy the following relation:0.2≦ETP/TP≦3.

A horizontal distance between two adjacent lens elements at height of ½entrance pupil diameter (HEP) is denoted by ED. The horizontal distance(ED) described above is in parallel with the optical axis of the opticalimage capturing system and particularly affects the corrected aberrationof common area of each field of view of light and the capability ofcorrecting optical path difference between each field of view of lightat the position of ½ entrance pupil diameter (HEP). The capability ofaberration correction may be enhanced if the horizontal distance becomesgreater, but the difficulty for manufacturing is also increased and thedegree of ‘miniaturization’ to the length of the optical image capturingsystem is restricted. Thus, it is essential to control the horizontaldistance (ED) between two specific adjacent lens elements at height of ½entrance pupil diameter (HEP).

In order to enhance the capability of aberration correction and reducethe difficulty for ‘miniaturization’ to the length of the optical imagecapturing system at the same time, it is particularly necessary tocontrol the ratio relation (ED/IN) of the horizontal distance (ED)between the two adjacent lens elements at height of ½ entrance pupildiameter (HEP) to the horizontal distance (IN) between the two adjacentlens elements on the optical axis. For example, the horizontal distancebetween the first lens element and the second lens element at height of½ entrance pupil diameter (HEP) is denoted by ED12. The horizontaldistance between the first lens element and the second lens element onthe optical axis is IN12. The ratio between both of them is ED12/IN12.The horizontal distance between the second lens element and the thirdlens element at height of ½ entrance pupil diameter (HEP) is denoted byED23. The horizontal distance between the second lens element and thethird lens element on the optical axis is IN23. The ratio between bothof them is ED23/IN23. The ratio relations of the horizontal distancesbetween other two adjacent lens elements in the optical image capturingsystem at height of ½ entrance pupil diameter (HEP) to the horizontaldistances between the two adjacent lens elements on the optical axis aredenoted in the similar way.

A horizontal distance in parallel with the optical axis from acoordinate point on the image-side surface of the sixth lens element atheight ½ HEP to the image plane is EBL. A horizontal distance inparallel with the optical axis from an axial point on the image-sidesurface of the sixth lens element to the image plane is BL. Theembodiments of the present invention enhance the capability ofaberration correction and reserve space for accommodating other opticalelements. The following relation may be satisfied: 0.2≦EBL/BL<1.1. Theoptical image capturing system may further include a light filtrationelement. The light filtration element is located between the sixth lenselement and the image plane. A distance in parallel with the opticalaxis from a coordinate point on the image-side surface of the sixth lenselement at height ½ HEP to the light filtration element is EIR. Adistance in parallel with the optical axis from an axial point on theimage-side surface of the sixth lens element to the light filtrationelement is PIR. The embodiments of the present invention may satisfy thefollowing relation: 0.1≦EIR/PIR≦1.1.

The height of optical system (HOS) may be reduced to achieve theminimization of the optical image capturing system when the absolutevalue of f1 is larger than f6 (|f1|>f6).

When |f2|+|f3|+|f4|+|f5| and |f1|+|f6| are satisfied with aboverelations, at least one of the second through fifth lens elements mayhave weak positive refractive power or weak negative refractive power.The weak refractive power indicates that an absolute value of the focallength of a specific lens element is greater than 10. When at least oneof the second through fifth lens elements has the weak positiverefractive power, the positive refractive power of the first lenselement can be shared, such that the unnecessary aberration will notappear too early. On the contrary, when at least one of the secondthrough fifth lens elements has the weak negative refractive power, theaberration of the optical image capturing system can be corrected andfine tuned.

The sixth lens element may have negative refractive power and a concaveimage-side surface. Hereby, the back focal length is reduced for keepingthe miniaturization, to miniaturize the lens element effectively. Inaddition, at least one of the object-side surface and the image-sidesurface of the sixth lens element may have at least one inflectionpoint, such that the angle of incident with incoming light from anoff-axis field of view can be suppressed effectively and the aberrationin the off-axis field of view can be corrected further.

BRIEF DESCRIPTION OF THE DRAWINGS

The detailed structure, operating principle and effects of the presentdisclosure will now be described in more details hereinafter withreference to the accompanying drawings that show various embodiments ofthe present disclosure as follows.

FIG. 1A is a schematic view of the optical image capturing systemaccording to the first embodiment of the present application.

FIG. 1B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the first embodimentof the present application.

FIG. 1C is a characteristic diagram of modulation transfer of a visiblelight according to the first embodiment of the present application.

FIG. 1D is a characteristic diagram of modulation transfer of infraredrays according to the first embodiment of the present application.

FIG. 2A is a schematic view of the optical image capturing systemaccording to the second embodiment of the present application.

FIG. 2B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the secondembodiment of the present application.

FIG. 2C is a characteristic diagram of modulation transfer of a visiblelight according to the second embodiment of the present application.

FIG. 2D is a characteristic diagram of modulation transfer of infraredrays according to the second embodiment of the present application.

FIG. 3A is a schematic view of the optical image capturing systemaccording to the third embodiment of the present application.

FIG. 3B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the third embodimentof the present application.

FIG. 3C is a characteristic diagram of modulation transfer of a visiblelight according to the third embodiment of the present application.

FIG. 3D is a characteristic diagram of modulation transfer of infraredrays according to the third embodiment of the present application.

FIG. 4A is a schematic view of the optical image capturing systemaccording to the fourth embodiment of the present application.

FIG. 4B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the fourthembodiment of the present application.

FIG. 4C is a characteristic diagram of modulation transfer of a visiblelight according to the fourth embodiment of the present application.

FIG. 4D is a characteristic diagram of modulation transfer of infraredrays according to the fourth embodiment of the present application.

FIG. 5A is a schematic view of the optical image capturing systemaccording to the fifth embodiment of the present application.

FIG. 5B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the fifth embodimentof the present application.

FIG. 5C is a characteristic diagram of modulation transfer of a visiblelight according to the fifth embodiment of the present application.

FIG. 5D is a characteristic diagram of modulation transfer of infraredrays according to the fifth embodiment of the present application.

FIG. 6A is a schematic view of the optical image capturing systemaccording to the sixth embodiment of the present application.

FIG. 6B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the sixth embodimentof the present application.

FIG. 6C is a characteristic diagram of modulation transfer of a visiblelight according to the sixth embodiment of the present application.

FIG. 6D is a characteristic diagram of modulation transfer of infraredrays according to the sixth embodiment of the present application.

FIG. 7A is a schematic view of the optical image capturing systemaccording to the seventh embodiment of the present application.

FIG. 7B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the seventhembodiment of the present application.

FIG. 7C is a characteristic diagram of modulation transfer of a visiblelight according to the seventh embodiment of the present application.

FIG. 7D is a characteristic diagram of modulation transfer of infraredrays according to the seventh embodiment of the present application.

FIG. 8A is a schematic view of the optical image capturing systemaccording to the eighth embodiment of the present application.

FIG. 8B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the eighthembodiment of the present application.

FIG. 8C is a characteristic diagram of modulation transfer of a visiblelight according to the eighth embodiment of the present application.

FIG. 8D is a characteristic diagram of modulation transfer of infraredrays according to the eighth embodiment of the present application.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

Reference will now be made in detail to the exemplary embodiments of thepresent disclosure, examples of which are illustrated in theaccompanying drawings. Therefore, it is to be understood that theforegoing is illustrative of exemplary embodiments and is not to beconstrued as limited to the specific embodiments disclosed, and thatmodifications to the disclosed exemplary embodiments, as well as otherexemplary embodiments, are intended to be included within the scope ofthe appended claims. These embodiments are provided so that thisdisclosure will be thorough and complete, and will fully convey theinventive concept to those skilled in the art. The relative proportionsand ratios of elements in the drawings may be exaggerated or diminishedin size for the sake of clarity and convenience in the drawings, andsuch arbitrary proportions are only illustrative and not limiting in anyway. The same reference numbers are used in the drawings and thedescription to refer to the same or like parts.

It will be understood that, although the terms ‘first’, ‘second’,‘third’, etc., may be used herein to describe various elements, theseelements should not be limited by these terms. The terms are used onlyfor the purpose of distinguishing one component from another component.Thus, a first element discussed below could be termed a second elementwithout departing from the teachings of embodiments. As used herein, theterm “or” includes any and all combinations of one or more of theassociated listed items.

An optical image capturing system, in order from an object side to animage side, includes a first, second, third, fourth, fifth and sixthlens elements with refractive power and an image plane. The opticalimage capturing system may further include an image sensing device whichis disposed on an image plane.

The optical image capturing system may use three sets of wavelengthswhich are 486.1 nm, 587.5 nm and 656.2 nm, respectively, wherein 587.5nm is served as the primary reference wavelength and a referencewavelength for retrieving technical features. The optical imagecapturing system may also use five sets of wavelengths which are 470 nm,510 nm, 555 nm, 610 nm and 650 nm, respectively, wherein 555 nm isserved as the primary reference wavelength and a reference wavelengthfor retrieving technical features.

A ratio of the focal length f of the optical image capturing system to afocal length fp of each of lens elements with positive refractive poweris PPR. A ratio of the focal length f of the optical image capturingsystem to a focal length fn of each of lens elements with negativerefractive power is NPR. A sum of the PPR of all lens elements withpositive refractive power is ΣPPR. A sum of the NPR of all lens elementswith negative refractive powers is ΣNPR. It is beneficial to control thetotal refractive power and the total length of the optical imagecapturing system when following conditions are satisfied:0.5≦ΣPPR/ΣNPR|≦15. Preferably, the following relation may be satisfied:1≦ΣPPR/|ΣNPR|≦3.0.

The optical image capturing system may further include an image sensingdevice which is disposed on an image plane. Half of a diagonal of aneffective detection field of the image sensing device (imaging height orthe maximum image height of the optical image capturing system) is HOI.A distance on the optical axis from the object-side surface of the firstlens element to the image plane is HOS. The following relations aresatisfied: HOS/HOI≦10 and 0.5≦HOS/f≦10. Preferably, the followingrelations may be satisfied: 1≦HOS/HOI≦5 and 1≦HOS/f≦7. Hereby, theminiaturization of the optical image capturing system can be maintainedeffectively, so as to be carried by lightweight portable electronicdevices.

In addition, in the optical image capturing system of the disclosure,according to different requirements, at least one aperture stop may bearranged for reducing stray light and improving the imaging quality.

In the optical image capturing system of the disclosure, the aperturestop may be a front or middle aperture. The front aperture is theaperture stop between a photographed object and the first lens element.The middle aperture is the aperture stop between the first lens elementand the image plane. If the aperture stop is the front aperture, alonger distance between the exit pupil and the image plane of theoptical image capturing system can be formed, such that more opticalelements can be disposed in the optical image capturing system and theefficiency of receiving images of the image sensing device can beraised. If the aperture stop is the middle aperture, the view angle ofthe optical image capturing system can be expended, such that theoptical image capturing system has the same advantage that is owned bywide angle cameras. A distance from the aperture stop to the image planeis InS. The following relation is satisfied: 0.2≦InS/HOS≦1.1. Hereby,features of maintaining the minimization for the optical image capturingsystem and having wide-angle are available simultaneously.

In the optical image capturing system of the disclosure, a distance fromthe object-side surface of the first lens element to the image-sidesurface of the sixth lens element is InTL. A sum of central thicknessesof all lens elements with refractive power on the optical axis is ΣTP.The following relation is satisfied: 0.1≦ΣTP/InTL≦0.9. Hereby, contrastratio for the image formation in the optical image capturing system anddefect-free rate for manufacturing the lens element can be givenconsideration simultaneously, and a proper back focal length is providedto dispose other optical components in the optical image capturingsystem.

A curvature radius of the object-side surface of the first lens elementis R1. A curvature radius of the image-side surface of the first lenselement is R2. The following relation is satisfied: 0.001≦|R1/R2|≦20.Hereby, the first lens element may have proper strength of the positiverefractive power, so as to avoid the longitudinal spherical aberrationto increase too fast. Preferably, the following relation may besatisfied: 0.01≦|R1/R2|<10.

A curvature radius of the object-side surface of the sixth lens elementis R11. A curvature radius of the image-side surface of the sixth lenselement is R12. The following relation is satisfied:−7<(R11−R12)/(R11+R12)<50. Hereby, the astigmatism generated by theoptical image capturing system can be corrected beneficially.

A distance between the first lens element and the second lens element onthe optical axis is IN12. The following relation is satisfied:IN12/f≦3.0. Hereby, the chromatic aberration of the lens elements can beimproved, such that the performance can be increased.

A distance between the fifth lens element and the sixth lens element onthe optical axis is IN56. The following relation is satisfied:IN56/f≦0.8. Hereby, the chromatic aberration of the lens elements can beimproved, such that the performance can be increased.

Central thicknesses of the first lens element and the second lenselement on the optical axis are TP1 and TP2, respectively. The followingrelation is satisfied: 0.1≦(TP1+IN12)/TP2≦10. Hereby, the sensitivityproduced by the optical image capturing system can be controlled, andthe performance can be increased.

Central thicknesses of the fifth lens element and the sixth lens elementon the optical axis are TP5 and TP6, respectively, and a distancebetween the aforementioned two lens elements on the optical axis isIN56. The following relation is satisfied: 0.1≦(TP6+IN56)/TP5≦10.Hereby, the sensitivity produced by the optical image capturing systemcan be controlled and the total height of the optical image capturingsystem can be reduced.

Central thicknesses of the second lens element, the third lens elementand the fourth lens element on the optical axis are TP2, TP3 and TP4,respectively. A distance between the second lens element and the thirdlens element on the optical axis is IN23. A distance between the thirdlens element and the fourth lens element on the optical axis is IN34. Adistance between the fourth lens element and the fifth lens element onthe optical axis is IN45. A distance on the optical axis from theobject-side surface of the first lens element to the image-side surfaceof the sixth lens element is InTL The following relation is satisfied:0.1≦TP4/(IN34+TP4+IN45)<1. Hereby, the aberration generated by theprocess of moving the incident light can be adjusted slightly layer uponlayer, and the total height of the optical image capturing system can bereduced.

In the optical image capturing system of the disclosure, a distanceperpendicular to the optical axis between a critical point C61 on theobject-side surface of the sixth lens element and the optical axis isHVT61. A distance perpendicular to the optical axis between a criticalpoint C62 on the image-side surface of the sixth lens element and theoptical axis is HVT62. A horizontal displacement distance on the opticalaxis from an axial point on the object-side surface of the sixth lenselement to the critical point C61 is SGC61. A horizontal displacementdistance on the optical axis from an axial point on the image-sidesurface of the sixth lens element to the critical point C62 is SGC62.The following relations may be satisfied: 0 mm≦HVT61≦3 mm, 0 mm<HVT62≦6mm, 0≦HVT61/HVT62, 0 mm≦|SGC61|≦0.5 mm, 0 mm<|SGC62|≦2 mm and0<|SGC62|/(|SGC62|+TP6)≦0.9. Hereby, the aberration in the off-axis viewfield can be corrected.

The optical image capturing system of the disclosure satisfies thefollowing relation: 0.2≦HVT62/HOI≦0.9. Preferably, the followingrelation may be satisfied: 0.3≦HVT62/HOI≦0.8. Hereby, the aberration ofsurrounding view field can be corrected.

The optical image capturing system of the disclosure satisfies thefollowing relation: 0≦HVT62/HOS≦0.5. Preferably, the following relationmay be satisfied: 0.2≦HVT62/HOS≦0.45. Hereby, the aberration ofsurrounding view field can be corrected.

In the optical image capturing system of the disclosure, a distance inparallel with an optical axis from an inflection point on theobject-side surface of the sixth lens element which is nearest to theoptical axis to an axial point on the object-side surface of the sixthlens element is denoted by SGI611. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thesixth lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the sixth lens element is denoted bySGI621. The following relations are satisfied: 0<SGI611/(SGI611+TP6)≦0.9and 0<SGI621/(SGI621+TP6)≦0.9. Preferably, the following relations maybe satisfied: 0.1≦SGI611/(SGI611+TP6)≦0.6 and0.1≦SGI621/(SGI621+TP6)≦0.6.

A distance in parallel with the optical axis from the inflection pointon the object-side surface of the sixth lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the sixth lens element is denoted by SGI612. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the sixth lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the sixth lenselement is denoted by SGI622. The following relations are satisfied:0<SGI612/(SGI612+TP6)≦0.9 and 0<SGI622/(SGI622+TP6)≦0.9. Preferably, thefollowing relations may be satisfied: 0.1≦SGI612/(SGI612+TP6)≦0.6 and0.1≦SGI622/(SGI622+TP6)≦0.6.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which isnearest to the optical axis and the optical axis is denoted by HIF611. Adistance perpendicular to the optical axis between an inflection pointon the image-side surface of the sixth lens element which is nearest tothe optical axis and an axial point on the image-side surface of thesixth lens element is denoted by HIF621. The following relations aresatisfied: 0.001 mm≦|HIF611|≦5 mm and 0.001 mm≦|HIF621|≦5 mm.Preferably, the following relations may be satisfied: 0.1mm≦|HIF611|≦3.5 mm and 1.5 mm≦|HIF621|≦3.5 mm.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thesecond nearest to the optical axis and the optical axis is denoted byHIF612. A distance perpendicular to the optical axis between an axialpoint on the image-side surface of the sixth lens element and aninflection point on the image-side surface of the sixth lens elementwhich is the second nearest to the optical axis is denoted by HIF622.The following relations are satisfied: 0.001 mm≦|HIF612|≦5 mm and 0.001mm≦|HIF622|≦5 mm. Preferably, the following relations may be satisfied:0.1 mm≦|HIF622|≦3.5 mm and 0.1 mm≦|HIF612|≦3.5 mm.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thethird nearest to the optical axis and the optical axis is denoted byHIF613. A distance perpendicular to the optical axis between an axialpoint on the image-side surface of the sixth lens element and aninflection point on the image-side surface of the sixth lens elementwhich is the third nearest to the optical axis is denoted by HIF623. Thefollowing relations are satisfied: 0.001 mm≦|HIF613|≦5 mm and 0.001mm≦|HIF623|≦5 mm. Preferably, the following relations may be satisfied:0.1 mm≦|HIF623|≦3.5 mm and 0.1 mm≦|HIF613|≦3.5 mm.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thefourth nearest to the optical axis and the optical axis is denoted byHIF614. A distance perpendicular to the optical axis between an axialpoint on the image-side surface of the sixth lens element and aninflection point on the image-side surface of the sixth lens elementwhich is the fourth nearest to the optical axis is denoted by HIF624.The following relations are satisfied: 0.001 mm≦|HIF614|≦5 mm and 0.001mm≦|HIF624|≦5 mm. Preferably, the following relations may be satisfied:0.1 mm≦|HIF624|≦3.5 mm and 0.1 mm≦|HIF614|≦3.5 mm.

In one embodiment of the optical image capturing system of the presentdisclosure, the chromatic aberration of the optical image capturingsystem can be corrected by alternatively arranging the lens elementswith large Abbe number and small Abbe number.

The above Aspheric formula is:

z=ch ²/[1+[1−(k+1)c ² h ²]^(0.5) ]+A4h ⁴ +A6h ⁶ +A8h ⁸ +A10h ¹⁰ +A12h ¹²+A14h ¹⁴ +A16h ¹⁶ +A18h ¹⁸ +A20h ²⁰+ . . .  (1),

where z is a position value of the position along the optical axis andat the height h which reference to the surface apex; k is the coniccoefficient, c is the reciprocal of curvature radius, and A4, A6, A8,A10, A12, A14, A16, A18, and A20 are high order aspheric coefficients.

The optical image capturing system provided by the disclosure, the lenselements may be made of glass or plastic material. If plastic materialis adopted to produce the lens elements, the cost of manufacturing willbe lowered effectively. If lens elements are made of glass, the heateffect can be controlled and the designed space arranged for therefractive power of the optical image capturing system can be increased.Besides, the object-side surface and the image-side surface of the firstthrough sixth lens elements may be aspheric, so as to obtain morecontrol variables. Comparing with the usage of traditional lens elementmade by glass, the number of lens elements used can be reduced and theaberration can be eliminated. Thus, the total height of the opticalimage capturing system can be reduced effectively.

In addition, in the optical image capturing system provided by thedisclosure, if the lens element has a convex surface, the surface of thelens element adjacent to the optical axis is convex in principle. If thelens element has a concave surface, the surface of the lens elementadjacent to the optical axis is concave in principle.

The optical image capturing system of the disclosure can be adapted tothe optical image capturing system with automatic focus if required.With the features of a good aberration correction and a high quality ofimage formation, the optical image capturing system can be used invarious application fields.

The optical image capturing system of the disclosure can include adriving module according to the actual requirements. The driving modulemay be coupled with the lens elements to enable the lens elementsproducing displacement. The driving module may be the voice coil motor(VCM) which is applied to move the lens to focus, or may be the opticalimage stabilization (OIS) which is applied to reduce the distortionfrequency owing to the vibration of the lens while shooting.

At least one of the first, second, third, fourth, fifth and sixth lenselements of the optical image capturing system of the disclosure mayfurther be designed as a light filtration element with a wavelength ofless than 500 nm according to the actual requirement. The lightfiltration element may be made by coating at least one surface of thespecific lens element characterized of the filter function, andalternatively, may be made by the lens element per se made of thematerial which is capable of filtering short wavelength.

According to the above embodiments, the specific embodiments withfigures are presented in detail as below.

The First Embodiment (Embodiment 1)

Please refer to FIG. 1A and FIG. 1B. FIG. 1A is a schematic view of theoptical image capturing system according to the first embodiment of thepresent application, FIG. 1B is longitudinal spherical aberrationcurves, astigmatic field curves, and an optical distortion curve of theoptical image capturing system in the order from left to right accordingto the first embodiment of the present application, FIG. 1C is acharacteristic diagram of modulation transfer of a visible lightaccording to the first embodiment of the present application, and FIG.1D is a characteristic diagram of modulation transfer of infrared raysaccording to the first embodiment of the present application. As shownin FIG. 1A, in order from an object side to an image side, the opticalimage capturing system includes a first lens element 110, an aperturestop 100, a second lens element 120, a third lens element 130, a fourthlens element 140, a fifth lens element 150, a sixth lens element 160, anIR-bandstop filter 180, an image plane 190, and an image sensing device192.

The first lens element 110 has negative refractive power and it is madeof plastic material. The first lens element 110 has a concaveobject-side surface 112 and a concave image-side surface 114, and bothof the object-side surface 112 and the image-side surface 114 areaspheric. The object-side surface 112 has two inflection points. Thethickness of the first lens element on the optical axis is TP1. Thethickness of the first lens element at height of ½ entrance pupildiameter (HEP) is denoted by ETP1.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the first lens element which is nearest tothe optical axis to an axial point on the object-side surface of thefirst lens element is denoted by SGI111. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thefirst lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the first lens element is denoted bySGI121. The following relations are satisfied: SGI111=−0.0031 mm and|SGI111|/(|SGI111|+TP1)=0.0016.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the first lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the first lens element is denoted by SGI112. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the first lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the first lenselement is denoted by SGI122. The following relations are satisfied:SGI112=1.3178 mm and |SGI112|/(|SGI112|+TP1)=0.4052.

A distance perpendicular to the optical axis from the inflection pointon the object-side surface of the first lens element which is nearest tothe optical axis to an axial point on the object-side surface of thefirst lens element is denoted by HIF111. A distance perpendicular to theoptical axis from the inflection point on the image-side surface of thefirst lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the first lens element is denoted byHIF121. The following relations are satisfied: HIF111=0.5557 mm andHIF111/HOI=0.1111.

A distance perpendicular to the optical axis from the inflection pointon the object-side surface of the first lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the first lens element is denoted by HIF112. A distance perpendicularto the optical axis from the inflection point on the image-side surfaceof the first lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the first lenselement is denoted by HIF122. The following relations are satisfied:HIF112=5.3732 mm and HIF112/HOI=1.0746.

The second lens element 120 has positive refractive power and it is madeof plastic material. The second lens element 120 has a convexobject-side surface 122 and a convex image-side surface 124, and both ofthe object-side surface 122 and the image-side surface 124 are aspheric.The object-side surface 122 has an inflection point. The thickness ofthe second lens element on the optical axis is TP2. The thickness of thesecond lens element at height of ½ entrance pupil diameter (HEP) isdenoted by ETP2.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the second lens element which is nearest tothe optical axis to an axial point on the object-side surface of thesecond lens element is denoted by SGI211. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thesecond lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the second lens element is denoted bySGI221. The following relations are satisfied: SGI211=0.1069 mm,|SGI211|/(|SGI211|+TP2)=0.0412, SGI221=0 mm and|SGI221|/(|SGI221|+TP2)=0.

A distance perpendicular to the optical axis from the inflection pointon the object-side surface of the second lens element which is nearestto the optical axis to an axial point on the object-side surface of thesecond lens element is denoted by HIF211. A distance perpendicular tothe optical axis from the inflection point on the image-side surface ofthe second lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the second lens element is denoted byHIF221. The following relations are satisfied: HIF211=1.1264 mm,HIF211/HOI=0.2253, HIF221=0 mm and HIF221/HOI=0.

The third lens element 130 has negative refractive power and it is madeof plastic material. The third lens element 130 has a concaveobject-side surface 132 and a convex image-side surface 134, and both ofthe object-side surface 132 and the image-side surface 134 are aspheric.The object-side surface 132 and the image-side surface 134 both have aninflection point. The thickness of the third lens element on the opticalaxis is TP3. The thickness of the third lens element at height of ½entrance pupil diameter (HEP) is denoted by ETP3.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the third lens element which is nearest tothe optical axis to an axial point on the object-side surface of thethird lens element is denoted by SGI311. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thethird lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the third lens element is denoted bySGI321. The following relations are satisfied: SGI311=−0.3041 mm,|SGI311|/(|SGI311|+TP3)=0.4445, SGI321=−0.1172 mm and|SGI321|/(|SGI321|+TP3)=0.2357.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the third lens element which isnearest to the optical axis and the optical axis is denoted by HIF311. Adistance perpendicular to the optical axis from the inflection point onthe image-side surface of the third lens element which is nearest to theoptical axis to an axial point on the image-side surface of the thirdlens element is denoted by HIF321. The following relations aresatisfied: HIF311=1.5907 mm, HIF311/HOI=0.3181, HIF321=1.3380 mm andHIF321/HOI=0.2676.

The fourth lens element 140 has positive refractive power and it is madeof plastic material. The fourth lens element 140 has a convexobject-side surface 142 and a concave image-side surface 144, and bothof the object-side surface 142 and the image-side surface 144 areaspheric. The object-side surface 142 has two inflection points and theimage-side surface 144 has an inflection point. The thickness of thefourth lens element on the optical axis is TP4. The thickness of thefourth lens element at height of ½ entrance pupil diameter (HEP) isdenoted by ETP4.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fourth lens element which is nearest tothe optical axis to an axial point on the object-side surface of thefourth lens element is denoted by SGI411. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thefourth lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the fourth lens element is denoted bySGI421. The following relations are satisfied: SGI411=0.0070 mm,|SGI411|/(|SGI411|+TP4)=0.0056, SGI421=0.0006 mm and|SGI421|/(|SGI421|+TP4)=0.0005.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fourth lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the fourth lens element is denoted by SGI412. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the fourth lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the fourth lenselement is denoted by SGI422. The following relations are satisfied:SGI412=−0.2078 mm and |SGI412|/(|SGI412|+TP4)=0.1439.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fourth lens element which isnearest to the optical axis and the optical axis is denoted by HIF411. Adistance perpendicular to the optical axis between the inflection pointon the image-side surface of the fourth lens element which is nearest tothe optical axis and the optical axis is denoted by HIF421. Thefollowing relations are satisfied: HIF411=0.4706 mm, HIF411/HOI=0.0941,HIF421=0.1721 mm and HIF421/HOI=0.0344.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fourth lens element which is thesecond nearest to the optical axis and the optical axis is denoted byHIF412. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the fourth lens elementwhich is the second nearest to the optical axis and the optical axis isdenoted by HIF422. The following relations are satisfied: HIF412=2.0421mm and HIF412/HOI=0.4084.

The fifth lens element 150 has positive refractive power and it is madeof plastic material. The fifth lens element 150 has a convex object-sidesurface 152 and a convex image-side surface 154, and both of theobject-side surface 152 and the image-side surface 154 are aspheric. Theobject-side surface 152 has two inflection points and the image-sidesurface 154 has an inflection point. The thickness of the fifth lenselement on the optical axis is TP5. The thickness of the fifth lenselement at height of ½ entrance pupil diameter (HEP) is denoted by ETP5.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fifth lens element which is nearest tothe optical axis to an axial point on the object-side surface of thefifth lens element is denoted by SGI511. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thefifth lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the fifth lens element is denoted bySGI521. The following relations are satisfied: SGI511=0.00364 mm,|SGI511|/(|SGI511|+TP5)=0.00338, SGI521=−0.63365 mm and|SGI521|/(|SGI521|+TP5)=0.37154.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fifth lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the fifth lens element is denoted by SGI512. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the fifth lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the fifth lenselement is denoted by SGI522. The following relations are satisfied:SGI512=−0.32032 mm and |SGI512|/(|SGI512|+TP5)=0.23009.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fifth lens element which is the thirdnearest to the optical axis to an axial point on the object-side surfaceof the fifth lens element is denoted by SGI513. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the fifth lens element which is the third nearest to the optical axisto an axial point on the image-side surface of the fifth lens element isdenoted by SGI523. The following relations are satisfied: SGI513=0 mm,|SGI513|/(|SGI513|+TP5)=0, SGI523=0 mm and |SGI523|/(|SGI523|+TP5)=0.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fifth lens element which is the fourthnearest to the optical axis to an axial point on the object-side surfaceof the fifth lens element is denoted by SGI514. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the fifth lens element which is the fourth nearest to the opticalaxis to an axial point on the image-side surface of the fifth lenselement is denoted by SGI524. The following relations are satisfied:SGI514=0 mm, |SGI514|/(|SGI514|+TP5)=0, SGI524=0 mm and|SGI524|/(|SGI524|+TP5)=0.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens element which isnearest to the optical axis and the optical axis is denoted by HIF511. Adistance perpendicular to the optical axis between the inflection pointon the image-side surface of the fifth lens element which is nearest tothe optical axis and the optical axis is denoted by HIF521. Thefollowing relations are satisfied: HIF511=0.28212 mm,HIF511/HOI=0.05642, HIF521=2.13850 mm and HIF521/HOI=0.42770.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens element which is thesecond nearest to the optical axis and the optical axis is denoted byHIF512. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the fifth lens elementwhich is the second nearest to the optical axis and the optical axis isdenoted by HIF522. The following relations are satisfied: HIF512=2.51384mm and HIF512/HOI=0.50277.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens element which is thethird nearest to the optical axis and the optical axis is denoted byHIF513. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the fifth lens elementwhich is the third nearest to the optical axis and the optical axis isdenoted by HIF523. The following relations are satisfied: HIF513=0 mm,HIF513/HOI=0, HIF523=0 mm and HIF523/HOI=0.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens element which is thefourth nearest to the optical axis and the optical axis is denoted byHIF514. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the fifth lens elementwhich is the fourth nearest to the optical axis and the optical axis isdenoted by HIF524. The following relations are satisfied: HIF514=0 mm,HIF514/HOI=0, HIF524=0 mm and HIF524/HOI=0.

The sixth lens element 160 has negative refractive power and it is madeof plastic material. The sixth lens element 160 has a concaveobject-side surface 162 and a concave image-side surface 164, and theobject-side surface 162 has two inflection points and the image-sidesurface 164 has an inflection point. Hereby, the angle of incident ofeach view field on the sixth lens element can be effectively adjustedand the spherical aberration can thus be improved. The thickness of thesixth lens element on the optical axis is TP6. The thickness of thesixth lens element at height of ½ entrance pupil diameter (HEP) isdenoted by ETP6.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the sixth lens element which is nearest tothe optical axis to an axial point on the object-side surface of thesixth lens element is denoted by SGI611. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thesixth lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the sixth lens element is denoted bySGI621. The following relations are satisfied: SGI611=−0.38558 mm,|SGI611|/(|SGI611|+TP6)=0.27212, SGI621=0.12386 mm and|SGI621|/(|SGI621|+TP6)=0.10722.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the sixth lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the sixth lens element is denoted by SGI612. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the sixth lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the sixth lenselement is denoted by SGI621. The following relations are satisfied:SGI612=−0.47400 mm, |SGI612|/(|SGI612|+TP6)=0.31488, SGI622=0 mm and|SGI622|/(|SGI622|+TP6)=0.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which isnearest to the optical axis and the optical axis is denoted by HIF611. Adistance perpendicular to the optical axis between the inflection pointon the image-side surface of the sixth lens element which is nearest tothe optical axis and the optical axis is denoted by HIF621. Thefollowing relations are satisfied: HIF611=2.24283 mm,HIF611/HOI=0.44857, HIF621=1.07376 mm and HIF621/HOI=0.21475.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thesecond nearest to the optical axis and the optical axis is denoted byHIF612. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the sixth lens elementwhich is the second nearest to the optical axis and the optical axis isdenoted by HIF622. The following relations are satisfied: HIF612=2.48895mm and HIF612/HOI=0.49779.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thethird nearest to the optical axis and the optical axis is denoted byHIF613. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the sixth lens elementwhich is the third nearest to the optical axis and the optical axis isdenoted by HIF623. The following relations are satisfied: HIF613=0 mm,HIF613/HOI=0, HIF623=0 mm and HIF623/HOI=0.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thefourth nearest to the optical axis and the optical axis is denoted byHIF614. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the sixth lens elementwhich is the fourth nearest to the optical axis and the optical axis isdenoted by HIF624. The following relations are satisfied: HIF614=0 mm,HIF614/HOI=0, HIF624=0 mm and HIF624/HOI=0.

In the first embodiment, a horizontal distance in parallel with theoptical axis from a coordinate point on the object-side surface of thefirst lens element at height ½ HEP to the image plane is ETL. Ahorizontal distance in parallel with the optical axis from a coordinatepoint on the object-side surface of the first lens element at height ½HEP to a coordinate point on the image-side surface of the sixth lenselement at height ½ HEP is EIN. The following relations are satisfied:ETL=19.304 mm, EIN=15.733 mm and EIN/ETL=0.815.

The first embodiment satisfies the following relations: ETP1=2.371 mm,ETP2=2.134 mm, ETP3=0.497 mm, ETP4=1.111 mm, ETP5=1.783 mm andETP6=1.404 mm. A sum of ETP1 to ETP6 described above SETP=9.300 mm.TP1=2.064 mm, TP2=2.500 mm, TP3=0.380 mm, TP4=1.186 mm, TP5=2.184 mm andTP6=1.105 mm. A sum of TP1 to TP6 described above STP=9.419 mm.SETP/STP=0.987. SETP/EIN=0.5911.

The present embodiment particularly controls the ratio relation (ETP/TP)of the thickness (ETP) of each lens element at height of ½ entrancepupil diameter (HEP) to the thickness (TP) of the lens element to whichthe surface belongs on the optical axis in order to achieve a balancebetween manufacturability and capability of aberration correction. Thefollowing relations are satisfied: ETP1/TP1=1.149, ETP2/TP2=0.854,ETP3/TP3=1.308, ETP4/TP4=0.936, ETP5/TP5=0.817 and ETP6/TP6=1.271.

The present embodiment controls a horizontal distance between each twoadjacent lens elements at height of ½ entrance pupil diameter (HEP) toachieve a balance between the degree of miniaturization for the lengthof the optical image capturing system HOS, the manufacturability and thecapability of aberration correction. The ratio relation (ED/IN) of thehorizontal distance (ED) between the two adjacent lens elements atheight of ½ entrance pupil diameter (HEP) to the horizontal distance(IN) between the two adjacent lens elements on the optical axis isparticularly controlled. The following relations are satisfied: ahorizontal distance in parallel with the optical axis between the firstlens element and the second lens element at height of ½ entrance pupildiameter (HEP) ED12=5.285 mm; a horizontal distance in parallel with theoptical axis between the second lens element and the third lens elementat height of ½ entrance pupil diameter (HEP) ED23=0.283 mm; a horizontaldistance in parallel with the optical axis between the third lenselement and the fourth lens element at height of ½ entrance pupildiameter (HEP) ED34=0.330 mm; a horizontal distance in parallel with theoptical axis between the fourth lens element and the fifth lens elementat height of ½ entrance pupil diameter (HEP) ED45=0.348 mm; a horizontaldistance in parallel with the optical axis between the fifth lenselement and the sixth lens element at height of ½ entrance pupildiameter (HEP) ED56=0.187 mm. A sum of ED12 to ED56 described above isdenoted as SED and SED=6.433 mm.

The horizontal distance between the first lens element and the secondlens element on the optical axis IN12=5.470 mm and ED12/IN12=0.966. Thehorizontal distance between the second lens element and the third lenselement on the optical axis IN23=0.178 mm and ED23/IN23=1.590. Thehorizontal distance between the third lens element and the fourth lenselement on the optical axis IN34=0.259 mm and ED34/IN34=1.273. Thehorizontal distance between the fourth lens element and the fifth lenselement on the optical axis IN45=0.209 mm and ED45/IN45=1.664. Thehorizontal distance between the fifth lens element and the sixth lenselement on the optical axis IN56=0.034 mm and ED56/IN56=5.557. A sum ofIN12 to IN56 described above is denoted as SIN. SIN=6.150 mm.SED/SIN=1.046.

The first embodiment also satisfies the following relations:ED12/ED23=18.685, ED23/ED34=0.857, ED34/ED45=0.947, ED45/ED56=1.859,IN12/IN23=30.746, IN23/IN34=0.686, IN34/IN45=1.239 and IN45/IN56=6.207.

A horizontal distance in parallel with the optical axis from acoordinate point on the image-side surface of the sixth lens element atheight ½ HEP to the image plane EBL=3.570 mm. A horizontal distance inparallel with the optical axis from an axial point on the image-sidesurface of the sixth lens element to the image plane BL=4.032 mm. Theembodiment of the present invention may satisfy the following relation:EBL/BL=0.8854. In the present invention, a distance in parallel with theoptical axis from a coordinate point on the image-side surface of thesixth lens element at height ½ HEP to the IR-bandstop filter EIR=1.950mm. A distance in parallel with the optical axis from an axial point onthe image-side surface of the sixth lens element to the IR-bandstopfilter PIR=2.121 mm. The following relation is satisfied: EIR/PIR=0.920.

The IR-bandstop filter 180 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 160 and the image plane 190.

In the optical image capturing system of the first embodiment, a focallength of the optical image capturing system is f, an entrance pupildiameter of the optical image capturing system is HEP, and half of amaximal view angle of the optical image capturing system is HAF. Thedetailed parameters are shown as below: f=4.075 mm, f/HEP=1.4,HAF=50.001° and tan(HAF)=1.1918.

In the optical image capturing system of the first embodiment, a focallength of the first lens element 110 is f1 and a focal length of thesixth lens element 160 is f6. The following relations are satisfied:f1=−7.828 mm, |f/f1|=0.52060, f6=−4.886 and |f1|>|f6|.

In the optical image capturing system of the first embodiment, focallengths of the second lens element 120 to the fifth lens element 150 aref2, f3, f4 and f5, respectively. The following relations are satisfied:|f2|+|f3|+|f4|+|f5|=95.50815 mm, |f1|+|f6|=12.71352 mm and|f2|+|f3|+|f4|+|f5|>|f1|+|f6|.

A ratio of the focal length f of the optical image capturing system to afocal length fp of each of lens elements with positive refractive poweris PPR. A ratio of the focal length f of the optical image capturingsystem to a focal length fn of each of lens elements with negativerefractive power is NPR. In the optical image capturing system of thefirst embodiment, a sum of the PPR of all lens elements with positiverefractive power is ΣPPR=f/f1+f/f3+f/f5=1.63290. A sum of the NPR of alllens elements with negative refractive powers isΣNPR=|f/f1|+|f/f3|+|f/f6|=1.51305, ΣPPR/|ΣNPR|=1.07921. The followingrelations are also satisfied: f/f2|=0.69101, |f/f3|=0.15834,|f/f4|=0.06883, |f/f5|=0.87305 and |f/f6|=0.83412.

In the optical image capturing system of the first embodiment, adistance from the object-side surface 112 of the first lens element tothe image-side surface 164 of the sixth lens element is InTL. A distancefrom the object-side surface 112 of the first lens element to the imageplane 190 is HOS. A distance from an aperture 100 to an image plane 190is InS. Half of a diagonal length of an effective detection field of theimage sensing device 192 is HOI. A distance from the image-side surface164 of the sixth lens element to the image plane 190 is BFL. Thefollowing relations are satisfied: InTL+BFL=HOS, HOS=19.54120 mm,HOI=5.0 mm, HOS/HOI=3.90824, HOS/f=4.7952, InS=11.685 mm andInS/HOS=0.59794.

In the optical image capturing system of the first embodiment, a totalcentral thickness of all lens elements with refractive power on theoptical axis is ETP. The following relations are satisfied: ΣTP=8.13899mm and ΣTP/InTL=0.52477. Hereby, contrast ratio for the image formationin the optical image capturing system and defect-free rate formanufacturing the lens element can be given considerationsimultaneously, and a proper back focal length is provided to disposeother optical components in the optical image capturing system.

In the optical image capturing system of the first embodiment, acurvature radius of the object-side surface 112 of the first lenselement is R1. A curvature radius of the image-side surface 114 of thefirst lens element is R2. The following relation is satisfied:|R1/R2|=8.99987. Hereby, the first lens element may have proper strengthof the positive refractive power, so as to avoid the longitudinalspherical aberration to increase too fast.

In the optical image capturing system of the first embodiment, acurvature radius of the object-side surface 162 of the sixth lenselement is R11. A curvature radius of the image-side surface 164 of thesixth lens element is R12. The following relation is satisfied:(R11−R12)/(R11+R12)=1.27780. Hereby, the astigmatism generated by theoptical image capturing system can be corrected beneficially.

In the optical image capturing system of the first embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relations are satisfied: ΣPP=f1+f3+f5=69.770 mm andf5/(f2+f4+f5)=0.067. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the first embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relations are satisfied: ΣNP=f1+f3+f6=−38.451 mm andf6/(f1+f3+f6)=0.127. Hereby, it is favorable for allocating the positiverefractive power of the sixth lens element 160 to other negative lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the first embodiment, adistance between the first lens element 110 and the second lens element120 on the optical axis is IN12. The following relations are satisfied:IN12=6.418 mm and IN12/f=1.57491. Hereby, the chromatic aberration ofthe lens elements can be improved, such that the performance can beincreased.

In the optical image capturing system of the first embodiment, adistance between the fifth lens element 150 and the sixth lens element160 on the optical axis is IN56. The following relations are satisfied:IN56=0.025 mm and IN56/f=0.00613. Hereby, the chromatic aberration ofthe lens elements can be improved, such that the performance can beincreased.

In the optical image capturing system of the first embodiment, centralthicknesses of the first lens element 110 and the second lens element120 on the optical axis are TP1 and TP2, respectively. The followingrelations are satisfied: TP1=1.934 mm, TP2=2.486 mm and(TP1+IN12)/TP2=3.36005. Hereby, the sensitivity produced by the opticalimage capturing system can be controlled, and the performance can beincreased.

In the optical image capturing system of the first embodiment, centralthicknesses of the fifth lens element 150 and the sixth lens element 160on the optical axis are TP5 and TP6, respectively, and a distancebetween the aforementioned two lens elements on the optical axis isIN56. The following relations are satisfied: TP5=1.072 mm, TP6=1.031 mmand (TP6+IN56)/TP5=0.98555. Hereby, the sensitivity produced by theoptical image capturing system can be controlled and the total height ofthe optical image capturing system can be reduced.

In the optical image capturing system of the first embodiment, adistance between the third lens element 130 and the fourth lens element140 on the optical axis is IN34. A distance between the fourth lenselement 140 and the fifth lens element 150 on the optical axis is IN45.The following relations are satisfied: IN34=0.401 mm, IN45=0.025 mm andTP4/(IN34+TP4+IN45)=0.74376. Hereby, the aberration generated by theprocess of moving the incident light can be adjusted slightly layer uponlayer, and the total height of the optical image capturing system can bereduced.

In the optical image capturing system of the first embodiment, adistance in parallel with an optical axis from a maximum effective halfdiameter position to an axial point on the object-side surface 152 ofthe fifth lens element is InRS51. A distance in parallel with an opticalaxis from a maximum effective half diameter position to an axial pointon the image-side surface 154 of the fifth lens element is InRS52. Acentral thickness of the fifth lens element 150 is TP5. The followingrelations are satisfied: InRS51=−0.34789 mm, InRS52=−0.88185 mm,|InRS51□/TP5=0.32458 and |InRS52□/TP5=0.82276. Hereby, it is favorablefor manufacturing and forming the lens element and for maintaining theminimization for the optical image capturing system.

In the optical image capturing system of the first embodiment, adistance perpendicular to the optical axis between a critical point C51on the object-side surface 152 of the fifth lens element and the opticalaxis is HVT51. A distance perpendicular to the optical axis between acritical point C52 on the image-side surface 154 of the fifth lenselement and the optical axis is HVT52. The following relations aresatisfied: HVT51=0.515349 mm and HVT52=0 mm.

In the optical image capturing system of the first embodiment, adistance in parallel with an optical axis from a maximum effective halfdiameter position to an axial point on the object-side surface 162 ofthe sixth lens element is InRS61. A distance in parallel with an opticalaxis from a maximum effective half diameter position to an axial pointon the image-side surface 164 of the sixth lens element is InRS62. Acentral thickness of the sixth lens element 160 is TP6. The followingrelations are satisfied: InRS61=−0.58390 mm, InRS62=0.41976 mm,|InRS61□/TP6=0.56616 and |InRS62□/TP6=0.40700. Hereby, it is favorablefor manufacturing and forming the lens element and for maintaining theminimization for the optical image capturing system.

In the optical image capturing system of the first embodiment, adistance perpendicular to the optical axis between a critical point C61on the object-side surface 162 of the sixth lens element and the opticalaxis is HVT61. A distance perpendicular to the optical axis between acritical point C62 on the image-side surface 164 of the sixth lenselement and the optical axis is HVT62. The following relations aresatisfied: HVT61=0 mm and HVT62=0 mm.

In the optical image capturing system of the first embodiment, thefollowing relation is satisfied: HVT51/HOI=0.1031. Hereby, theaberration of surrounding view field can be corrected.

In the optical image capturing system of the first embodiment, thefollowing relation is satisfied: HVT51/HOS=0.02634. Hereby, theaberration of surrounding view field can be corrected.

In the optical image capturing system of the first embodiment, thesecond lens element 120, the third lens element 130 and the sixth lenselement 160 have negative refractive power. An Abbe number of the secondlens element is NA2. An Abbe number of the third lens element is NA3. AnAbbe number of the sixth lens element is NA6. The following relation issatisfied: NA6/NA2≦1. Hereby, the chromatic aberration of the opticalimage capturing system can be corrected.

In the optical image capturing system of the first embodiment, TVdistortion and optical distortion for image formation in the opticalimage capturing system are TDT and ODT, respectively. The followingrelations are satisfied: |TDT|=2.124% and |ODT|=5.076%.

In the optical image capturing system of the present embodiment,contrast transfer rates of modulation transfer with spatial frequenciesof 55 cycles/mm of a visible light at the optical axis on the imageplane, 0.3 HOI and 0.7 HOI are respectively denoted by MTFE0, MTFE3 andMTFE7. The following relations are satisfied: MTFE0 is about 0.84, MTFE3is about 0.84 and MTFE7 is about 0.75. The contrast transfer rates ofmodulation transfer with spatial frequencies of 110 cycles/mm of avisible light at the optical axis on the image plane, 0.3 HOI and 0.7HOI are respectively denoted by MTFQ0, MTFQ3 and MTFQ7. The followingrelations are satisfied: MTFQ0 is about 0.66, MTFQ3 is about 0.65 andMTFQ7 is about 0.51. The contrast transfer rates of modulation transferwith spatial frequencies of 220 cycles/mm (MTF values) at the opticalaxis on the image plane, 0.3 HOI and 0.7 HOI are respectively denoted byMTFH0, MTFH3 and MTFH7. The following relations are satisfied: MTFH0 isabout 0.17, MTFH3 is about 0.07 and MTFH7 is about 0.14.

In the optical image capturing system of the present embodiment, whenthe infrared wavelength 850 nm is applied to focus on the image plane,contrast transfer rates of modulation transfer with a spatial frequency(55 cycles/mm) (MTF values) of the image at the optical axis on theimage plane, 0.3 HOI and 0.7 HOI are respectively denoted by MTFI0,MTFI3 and MTFI7. The following relations are satisfied: MTFI0 is about0.81, MTFI3 is about 0.8 and MTFI7 is about 0.15.

Please refer to the following Table 1 and Table 2.

The detailed data of the optical image capturing system of the firstembodiment is as shown in Table 1.

TABLE 1 Data of the optical image capturing system f = 4.075 mm, f/HEP =1.4, HAF = 50.000 deg Surface Focal # Curvature Radius ThicknessMaterial Index Abbe # length 0 Object Plano Plano 1 Lens 1 −40.996257041.934 Plastic 1.515 56.55 −7.828 2 4.555209289 5.923 3 Ape. stop Plano0.495 4 Lens 2 5.333427366 2.486 Plastic 1.544 55.96 5.897 5−6.781659971 0.502 6 Lens 3 −5.697794287 0.380 Plastic 1.642 22.46−25.738 7 −8.883957518 0.401 8 Lens 4 13.19225664 1.236 Plastic 1.54455.96 59.205 9 21.55681832 0.025 10 Lens 5 8.987806345 1.072 Plastic1.515 56.55 4.668 11 −3.158875374 0.025 12 Lens 6 −29.46491425 1.031Plastic 1.642 22.46 −4.886 13 3.593484273 2.412 14 IR-bandstop Plano0.200 1.517 64.13 filter 15 Plano 1.420 16 Image plane Plano Referencewavelength (d−line) = 555nm, shield position: clear aperture (CA) of thefirst plano = 5.800 mm; clear aperture (CA) of the third plano the fifthplanoAs for the parameters of the aspheric surfaces of the first embodiment,reference is made to Table 2.

TABLE 2 Aspheric Coefficients Surface # 1 2 4 5 6 7 8 k  4.310876E+01−4.707622E+00  2.616025E+00  2.445397E+00  5.645686E+00 −2.117147E+01−5.287220E+00 A4  7.054243E−03  1.714312E−02 −8.377541E−03 −1.789549E−02−3.379055E−03 −1.370959E−02 −2.937377E−02 A6 −5.233264E−04 −1.502232E−04−1.838068E−03 −3.657520E−03 −1.225453E−03  6.250200E−03  2.743532E−03 A8 3.077890E−05 −1.359611E−04  1.233332E−03 −1.131622E−03 −5.979572E−03−5.854426E−03 −2.457574E−03 A10 −1.260650E−06  2.680747E−05−2.390895E−03  1.390351E−03  4.556449E−03  4.049451E−03  1.874319E−03A12  3.319093E−08 −2.017491E−06  1.998555E−03 −4.152857E−04−1.177175E−03 −1.314592E−03 −6.013661E−04 A14 −5.051600E−10 6.604615E−08 −9.734019E−04  5.487286E−05  1.370522E−04  2.143097E−04 8.792480E−05 A16  3.380000E−12 −1.301630E−09  2.478373E−04−2.919339E−06 −5.974015E−06 −1.399894E−05 −4.770527E−06 Surface # 9 1011 12 13 k  6.200000E+01 −2.114008E+01 −7.699904E+00 −6.155476E+01−3.120467E−01 A4 −1.359965E−01 −1.263831E−01 −1.927804E−02 −2.492467E−02−3.521844E−02 A6  6.628518E−02  6.965399E−02  2.478376E−03 −1.835360E−03 5.629654E−03 A8 −2.129167E−02 −2.116027E−02  1.438785E−03  3.201343E−03−5.466925E−04 A10  4.396344E−03  3.819371E−03 −7.013749E−04−8.990757E−04  2.231154E−05 A12 −5.542899E−04 −4.040283E−04 1.253214E−04  1.245343E−04  5.548990E−07 A14  3.768879E−05 2.280473E−05 −9.943196E−06 −8.788363E−06 −9.396920E−08 A16−1.052467E−06 −5.165452E−07  2.898397E−07  2.494302E−07  2.728360E−09

Table 1 is the detailed structure data to the first embodiment in FIG.1A, wherein the unit of the curvature radius, the thickness, thedistance, and the focal length is millimeters (mm). Surfaces 0-16illustrate the surfaces from the object side to the image plane in theoptical image capturing system. Table 2 is the aspheric coefficients ofthe first embodiment, wherein k is the conic coefficient in the asphericsurface formula, and A1-A20 are the first to the twentieth orderaspheric surface coefficient. Besides, the tables in the followingembodiments are referenced to the schematic view and the aberrationgraphs, respectively, and definitions of parameters in the tables areequal to those in the Table 1 and the Table 2, so the repetitiousdetails will not be given here.

The Second Embodiment (Embodiment 2)

Please refer to FIG. 2A, FIG. 2B, FIGS. 2C, and 2D. FIG. 2A is aschematic view of the optical image capturing system according to thesecond embodiment of the present application, FIG. 2B is longitudinalspherical aberration curves, astigmatic field curves, and an opticaldistortion curve of the optical image capturing system in the order fromleft to right according to the second embodiment of the presentapplication, FIG. 2C is a characteristic diagram of modulation transferof a visible light according to the second embodiment of the presentapplication, and FIG. 2D is a characteristic diagram of modulationtransfer of infrared rays according to the second embodiment of thepresent application. As shown in FIG. 2A, in order from an object sideto an image side, the optical image capturing system includes anaperture stop 200, a first lens element 210, a second lens element 220,a third lens element 230, a fourth lens element 240, a fifth lenselement 250, a sixth lens element 260, an IR-bandstop filter 280, animage plane 290, and an image sensing device 292.

The first lens element 210 has positive refractive power and it is madeof plastic material. The first lens element 210 has a convex object-sidesurface 212 and a convex image-side surface 214, and both of theobject-side surface 212 and the image-side surface 214 are aspheric. Theobject-side surface 212 has one inflection point.

The second lens element 220 has negative refractive power and it is madeof plastic material. The second lens element 220 has a convexobject-side surface 222 and a concave image-side surface 224, and bothof the object-side surface 222 and the image-side surface 224 areaspheric and have one inflection point.

The third lens element 230 has positive refractive power and it is madeof plastic material. The third lens element 230 has a convex object-sidesurface 232 and a convex image-side surface 234, and both of theobject-side surface 232 and the image-side surface 234 are aspheric. Theobject-side surface 232 has two inflection points and the image-sidesurface 234 has one inflection point.

The fourth lens element 240 has positive refractive power and it is madeof plastic material. The fourth lens element 240 has a concaveobject-side surface 242 and a convex image-side surface 244, and both ofthe object-side surface 242 and the image-side surface 244 are asphericand have one inflection point.

The fifth lens element 250 has positive refractive power and it is madeof plastic material. The fifth lens element 250 has a convex object-sidesurface 252 and a convex image-side surface 254, and both of theobject-side surface 252 and the image-side surface 254 are aspheric. Theobject-side surface 252 has three inflection points and the image-sidesurface 254 has two inflection points.

The sixth lens element 260 has negative refractive power and it is madeof plastic material. The sixth lens element 260 has a convex object-sidesurface 262 and a concave image-side surface 264. The object-sidesurface 262 and the image-side surface 264 both have one inflectionpoint. Hereby, the back focal length is reduced to miniaturize the lenselement effectively. In addition, the angle of incident with incominglight from an off-axis view field can be suppressed effectively and theaberration in the off-axis view field can be corrected further.

The IR-bandstop filter 280 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 260 and the image plane 290.

In the optical image capturing system of the second embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relations are satisfied: ΣPP=24.823 mm andf1/ΣPP=0.368. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the second embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relation is satisfied: ΣNP=−14.739 mm andf2/ΣNP=0.874. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 3 and Table 4.

The detailed data of the optical image capturing system of the secondembodiment is as shown in Table 3.

TABLE 3 Data of the optical image capturing system f = 3.937 mm; f/HEP =1.6; HAF = 45 deg Surface Focal # Curvature Radius Thickness MaterialIndex Abbe # length 0 Object Plano At infinity 1 Ape. stop Plano −0.0302 Lens 1 5.431932967 0.800 Plastic 1.544 55.96 9.146 3 −59.056473810.000 4 1E+18 0.187 5 Lens 2 3.652087066 0.325 Plastic 1.642 22.46−12.880 6 2.451151358 0.271 7 Lens 3 7.566940154 0.845 Plastic 1.54455.96 8.572 8 −11.80094423 0.329 9 Lens 4 −2.295901061 0.845 Plastic1.544 55.96 3.190 10 −1.119543698 0.050 11 Lens 5 10.27776314 0.375Plastic 1.642 22.46 3.915 12 −3.317200075 0.050 13 Lens 6 7.644327590.400 Plastic 1.642 22.46 −1.859 14 1.018940222 0.787 15 IR-bandstopPlano 0.420 BK_7 1.517 64.13 filter 16 Plano 0.930 17 Image plane Plano0.000 Reference wavelength (d-line) = 555 nm shield position: clearaperture (CA) of the fourth plano = 1.320 mmAs for the parameters of the aspheric surfaces of the second embodiment,reference is made to Table 4.

TABLE 4 Aspheric Coefficients Surface # 2 3 5 6 7 8 9 k −9.672016E+00−8.999884E+01 −5.633964E+01 −4.714524E+00  1.525891E+01 −6.840624E+01−1.307354E+00 A4 −3.521377E−02 −6.990443E−02  3.786252E−03 −6.927918E−02−2.635941E−02 −4.599674E−02 −4.241518E−02 A6  3.817781E−01  9.589564E−02−1.233273E−01  5.626954E−02  −3.136161E−02  1.279117E−02  7.256388E−02A8 −1.484518E+00 −1.556220E−01  1.647475E−01 −7.572008E−02  5.220172E−02−2.129193E−02 −1.098840E−01 A10  2.966758E+00  1.388592E−01−1.808940E−01  6.171903E−02 −5.166506E−02  8.602254E−03  8.200036E−02A12 −3.376212E+00 −7.145006E−02  1.260316E−01 −3.031100E−02 2.412782E−02 −1.766672E−04 −2.905300E−02 A14  2.204154E+00 1.870940E−02 −4.963681E−02  7.719855E−03 −5.121586E−03 −4.439865E−04 4.887458E−03 A16 −7.692417E−01 −1.935232E−03  7.832566E−03−7.730803E−04  4.029040E−04  6.166007E−05 −3.155171E−04 A18 1.112092E−01  0.000000E+00  0.000000E+00  0.000000E+00  0.000000E+00 0.000000E+00  0.000000E+00 A20  0.000000E+00  0.000000E+00 0.000000E+00  0.000000E+00  0.000000E+00  0.000000E+00  0.000000E+00Surface # 10 11 12 13 14 k −1.601042E+00 −1.098051E+01 −7.388353E+01−8.727475E+01 −4.455130E+00 A4  4.247898E−03 −1.129775E−01 −3.259847E−02 1.106529E−01  7.145430E−03 A6  2.363136E−02  1.336945E−01  9.674594E−02−6.300834E−02 −1.060819E−02 A8 −5.041524E−02 −6.380262E−02 −4.945470E−02 1.676739E−02  2.418114E−03 A10  3.524922E−02  1.689788E−02 1.168008E−02 −2.526489E−03 −2.295706E−04 A12 −1.104615E−02−2.896370E−03 −1.473678E−03  2.201090E−04  4.822450E−06 A14 1.606093E−03  3.055564E−04  9.685603E−05 −1.026023E−05  6.066178E−07A16 −8.644267E−05 −1.466646E−05 −2.622410E−06  1.948524E−07−3.061311E−08

In the second embodiment, the presentation of the aspheric surfaceformula is similar to that in the first embodiment. Besides, thedefinitions of parameters in following tables are equal to those in thefirst embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 3 and Table 4.

Second embodiment (Primary reference wavelength = 555 nm) ETP1 ETP2 ETP3ETP4 ETP5 ETP6 0.562 0.519 0.660 0.624 0.302 0.644 ETP1/TP1 ETP2/TP2ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 0.703 1.596 0.781 0.739 0.805 1.610ETL EBL EIN EIR PIR EIN/ETL 6.502 1.717 4.785 0.367 0.787 0.736 SETP/EINEIR/PIR SETP STP SETP/STP BL 0.692 0.466 3.311 3.590 0.922 2.137 ED12ED23 ED34 ED45 ED56 EBL/BL 0.261 0.145 0.135 0.679 0.254 0.8035 SED SINSED/SIN ED12/ED23 ED23/ED34 ED34/ED45 1.474 0.887 1.662 1.802 1.0720.199 ED12/IN12 ED23/IN23 ED34/IN34 ED45/IN45 ED56/IN56 ED45/ED56 1.3990.535 0.410 13.578 5.076 2.675 | f/f1 | | f/f2 | | f/f3 | | f/f4 | |f/f5 | | f/f6 | 0.43046 0.30567 0.45928 1.23408 1.00570 2.11732 Σ PPR ΣNPR Σ PPR/| Σ NPR | IN12/f IN56/f TP4/(IN34 + TP4 + IN45) 3.129512.42299 1.29159 0.04738 0.01270 0.69014 | f1/f2 | | f2/f3 | (TP1 +IN12)/TP2 (TP6 + IN56)/TP5 0.71012 1.50251 3.03554 1.20000 HOS InTLHOS/HOI InS/HOS ODT % TDT % 6.61378 4.47667 1.65345 0.99544 1.602440.81026 HVT51 HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS 1.75224 0.918182.88708 2.48885 0.62221 0.37631 TP2/TP3 TP3/TP4 InRS61 InRS62 | InRS61|/TP6 | InRS62 |/TP6 0.38462 1.00000 0.38536 0.47412 0.96341 1.18531MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.87 0.83 0.76 0.71 0.54 0.42 MTFI0MTFI3 MTFI7 0.51 0.43 0.46

The following contents may be deduced from Table 3 and Table 4.

Related inflection point values of second embodiment (Primary referencewavelength: 555 nm) HIF111 0.9362 HIF111/HOI 0.2341 SGI111 0.0758 |SGI111 | /( | SGI111 | + TP1) 0.0865 HIF211 0.4711 HIF211/HOI 0.1178SGI211 0.0246 | SGI211 | /( | SGI211 | + TP2) 0.0704 HIF221 0.6988HIF221/HOI 0.1747 SGI211 0.0801 | SGI221 | /( | SGI221 | + TP2) 0.1978HIF311 0.5902 HIF311/HOI 0.1476 SGI311 0.0196 | SGI311 | /( | SGI311 | +TP3) 0.0227 HIF312 1.4676 HIF312/HOI 0.3669 SGI312 −0.0375 | SGI312 | /(| SGI312 | + TP3) 0.0425 HIF321 1.7134 HIF321/HOI 0.4283 SGI321 −0.4831| SGI321 | /( | SGI321 | + TP3) 0.3638 HIF411 1.2088 HIF411/HOI 0.3022SGI411 −0.3504 | SGI411 | /( | SGI411 | + TP4) 0.2931 HIF421 1.3434HIF421/HOI 0.3359 SGI421 −0.6799 | SGI421 | /( | SGI421 | + TP4) 0.4459HIF511 0.3093 HIF511/HOI 0.0773 SGI511 0.0037 | SGI511 | /( | SGI511 | +TP5) 0.0098 HIF512 0.6358 HIF512/HOI 0.1589 SGI512 0.0083 | SGI512 | /(| SGI512 | + TP5) 0.0217 HIF513 1.4247 HIF513/HOI 0.3562 SGI513 0.0828 |SGI513 | /( | SGI513 | + TP5) 0.1808 HIF521 0.5283 HIF521/HOI 0.1321SGI521 −0.0320 | SGI521 | /( | SGI521 | + TP5) 0.0787 HIF522 1.5332HIF522/HOI 0.3833 SGI522 0.0524 | SGI522 | /( | SGI522 | + TP5) 0.1226HIF611 1.2057 HIF611/HOI 0.3014 SGI611 0.1692 | SGI611 | /( | SGI611 | +TP6) 0.2973 HIF621 0.9885 HIF621/HOI 0.2471 SGI621 0.3121 | SGI621 | /(| SGI621 | + TP6) 0.4383

The Third Embodiment (Embodiment 3)

Please refer to FIG. 3A, FIG. 3B, FIGS. 3C, and 3D. FIG. 3A is aschematic view of the optical image capturing system according to thethird embodiment of the present application, FIG. 3B is longitudinalspherical aberration curves, astigmatic field curves, and an opticaldistortion curve of the optical image capturing system in the order fromleft to right according to the third embodiment of the presentapplication, FIG. 3C is a characteristic diagram of modulation transferof a visible light according to the third embodiment of the presentapplication, and FIG. 3D is a characteristic diagram of modulationtransfer of infrared rays according to the third embodiment of thepresent application. As shown in FIG. 3A, in order from an object sideto an image side, the optical image capturing system includes anaperture stop 300, a first lens element 310, a second lens element 320,a third lens element 330, a fourth lens element 340, a fifth lenselement 350, a sixth lens element 360, an IR-bandstop filter 380, animage plane 390, and an image sensing device 392.

The first lens element 310 has positive refractive power and it is madeof plastic material. The first lens element 310 has a convex object-sidesurface 312 and a convex image-side surface 314, and both of theobject-side surface 312 and the image-side surface 314 are aspheric. Theobject-side surface 312 has one inflection point.

The second lens element 320 has negative refractive power and it is madeof plastic material. The second lens element 320 has a convexobject-side surface 322 and a concave image-side surface 324, and bothof the object-side surface 322 and the image-side surface 324 areaspheric and have one inflection point.

The third lens element 330 has positive refractive power and it is madeof plastic material. The third lens element 330 has a convex object-sidesurface 332 and a convex image-side surface 334, and both of theobject-side surface 332 and the image-side surface 334 are aspheric. Theobject-side surface 332 has two inflection points and the image-sidesurface 334 has one inflection point.

The fourth lens element 340 has positive refractive power and it is madeof plastic material. The fourth lens element 340 has a concaveobject-side surface 342 and a convex image-side surface 344, and both ofthe object-side surface 342 and the image-side surface 344 are asphericand have one inflection point.

The fifth lens element 350 has positive refractive power and it is madeof plastic material. The fifth lens element 350 has a convex object-sidesurface 352 and a convex image-side surface 354, and both of theobject-side surface 352 and the image-side surface 354 are aspheric. Theobject-side surface 352 has three inflection points and the image-sidesurface 354 has two inflection points.

The sixth lens element 360 has negative refractive power and it is madeof plastic material. The sixth lens element 360 has a convex object-sidesurface 362 and a concave image-side surface 364. The object-sidesurface 362 and the image-side surface 364 both have one inflectionpoint. Hereby, the back focal length is reduced to miniaturize the lenselement effectively. In addition, the angle of incident with incominglight from an off-axis view field can be suppressed effectively and theaberration in the off-axis view field can be corrected further.

The IR-bandstop filter 380 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 360 and the image plane 390.

In the optical image capturing system of the third embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relation is satisfied: ΣPP=26.143 mm andf1/ΣPP=0.327. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the third embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relation is satisfied: ΣNP=−15.530 mm andf2/ΣNP=0.883. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 5 and Table 6.

The detailed data of the optical image capturing system of the thirdembodiment is as shown in Table 5.

TABLE 5 Data of the optical image capturing system f = 3.937 mm; f/HEP =1.7 ; HAF = 45 deg Surface Abbe Focal # Curvature Radius ThicknessMaterial Index # length 0 Object Plano At infinity 1 Ape. Stop Plano0.000 2 Lens 1 5.169903814 0.712 Plastic 1.544 55.96 8.539 3−45.42943691 0.000 4 1E+18 0.211 5 Lens 2 4.312166753 0.325 Plastic1.642 22.46 −13.718 6 2.817042334 0.256 7 Lens 3 8.362517397 0.818Plastic 1.544 55.96 10.711 8 −18.81195994 0.313 9 Lens 4 −2.4234400930.845 Plastic 1.544 55.96 3.243 10 −1.149443343 0.050 11 Lens 59.162177873 0.375 Plastic 1.642 22.46 3.650 12 −3.134369669 0.050 13Lens 6 6.946440551 0.400 Plastic 1.642 22.46 −1.812 14 0.98103664 0.78915 IR-bandstop Plano 0.420 BK_7 1.517 64.13 filter 16 Plano 0.930 17Imag plane Plano 0.000 Reference wavelength (d-line) = 555 nm, shieldposition: clear aperture (CA) of the fourth plano 1.320 mm;As for the parameters of the aspheric surfaces of the third embodiment,reference is made to Table 6.

TABLE 6 Aspheric Coefficients Surface # 2 3 5 6 7 8 9 k −1.572532E+01−9.000000E+01 −5.633867E+01 −4.758089E+00  1.714587E+01 −6.848079E+01−1.793537E+00 A4  1.002044E−03 −5.249100E−02 −1.686934E−02 −5.515861E−02−3.197501E−02 −3.457311E−02 −1.459514E−02 A6  1.505108E−01  5.038347E−02−3.330964E−02  5.246710E−02 −2.159255E−02 −1.675423E−02  3.170342E−03 A8−7.782919E−01 −1.126735E−01 −3.729597E−02 −9.670282E−02  4.525153E−02 1.847706E−02 −3.471447E−02 A10  1.825341E+00  1.184496E−01 5.787204E−02 8.998724E−02 −5.364854E−02 −2.074983E−02  4.179847E−02 A12−2.375497E+00 −7.174435E−02 −3.377244E−02 −4.796924E−02  2.775821E−02 1.179786E−02 −1.745624E−02 A14  1.752540E+00  2.219379E−02 5.702894E−03  1.316165E−02 −6.319254E−03 −2.998550E−03  3.140494E−03A16 −6.872584E−01 −2.808535E−03  2.280582E−04 −1.414714E−03 5.309939E−04  2.829616E−04 −2.076534E−04 A18  1.112092E−01 0.000000E+00  0.000000E+00  0.000000E+00  0.000000E+00  0.000000E+00 0.000000E+00 A20  0.000000E+00  0.000000E+00  0.000000E+00 0.000000E+00  0.000000E+00  0.000000E+00  0.000000E+00 Surface # 10 1112 13 14 k −1.669744E+00 −1.096511E+01 −7.387719E+01 −8.727465E+01−4.666060E+00 A4 −1.343259E−02 −1.105515E−01  8.628830E−03  1.241938E−01 8.444511E−03 A6  2.793947E−02  1.281840E−01  6.673158E−02 −7.413657E−02−1.151423E−02 A8 −5.015793E−02 −5.899583E−02 −4.046608E−02  2.093288E−02 2.623298E−03 A10  3.711693E−02  1.389646E−02  1.052552E−02−3.311907E−03 −2.401538E−04 A12 −1.207648E−02 −1.884601E−03−1.453761E−03  2.989195E−04  3.592605E−06 A14  1.794063E−03 1.370642E−04  1.048481E−04 −1.428779E−05  7.639957E−07 A16−9.816403E−05 −3.933133E−06 −3.116621E−06  2.772602E−07 −3.545101E−08A18  0.000000E+00  0.000000E+00  0.000000E+00  0.000000E+00 0.000000E+00 A20  0.000000E+00  0.000000E+00  0.000000E+00 0.000000E+00  0.000000E+00

The presentation of the aspheric surface formula in the third embodimentis similar to that in the first embodiment. Besides, the definitions ofparameters in following tables are equal to those in the firstembodiment so the repetitious details will not be given here.

The following contents may be deduced from Table 5 and Table 6.

The following contents may be deduced from Table 5 and Table 6.

Related inflection point values of third embodiment (Primary referencewavelength: 555 nm) HIF111 0.8693 HIF111/HOI 0.2173 SGI111 0.0684 |SGI111 | /( | SGI111 | + TP1) 0.0876 HIF211 0.4729 HIF211/HOI 0.1182SGI211 0.0214 | SGI211 | /( | SGI211 | + TP2) 0.0616 HIF221 0.6955HIF221/HOI 0.1739 SGI221 0.0710 | SGI221 | /( | SGI221 | + TP2) 0.1792HIF311 0.5457 HIF311/HOI 0.1364 SGI311 0.0150 | SGI311 | /( | SGI311 | +TP3) 0.0180 HIF312 1.4176 HIF312/HOI 0.3544 SGI312 −0.0495 | SGI312 | /(| SGI312 | + TP3) 0.0571 HIF321 1.7332 HIF321/HOI 0.4333 SGI321 −0.4815| SGI321 | /( | SGI321 | + TP3) 0.3705 HIF411 1.1480 HIF411/HOI 0.2870SGI411 −0.2891 | SGI411 | /( | SGI411 | + TP4) 0.2549 HIF421 1.2507HIF421/HOI 0.3127 SGI421 −0.5998 | SGI421 | /( | SGI421 | + TP4) 0.4151HIF511 0.3402 HIF511/HOI 0.0851 SGI511 0.0050 | SGI511 | /( | SGI511 | +TP5) 0.0132 HIF512 0.6240 HIF512/HOI 0.1560 SGI512 0.0106 | SGI512 | /(| SGI512 | + TP5) 0.0274 HIF513 1.3820 HIF513/HOI 0.3455 SGI513 0.0774 |SGI513 | /( | SGI513 | + TP5) 0.1710 HIF521 0.4443 HIF521/HOI 0.1111SGI521 −0.0237 | SGI521 | /( | SGI521 | + TP5) 0.0595 HIF522 1.5088HIF522/HOI 0.3772 SGI522 0.0785 | SGI522 | /( | SGI522 | + TP5) 0.1730HIF611 1.1963 HIF611/HOI 0.2991 SGI611 0.1788 | SGI611 | /( | SGI611 | +TP6) 0.3089 HIF621 0.9689 HIF621/HOI 0.2422 SGI621 0.3046 | SGI621 | /(| SGI621 | + TP6) 0.4323

The Fourth Embodiment (Embodiment 4)

Please refer to FIG. 4A, FIG. 4B, FIGS. 4C, and 4D. FIG. 4A is aschematic view of the optical image capturing system according to thefourth embodiment of the present application, FIG. 4B is longitudinalspherical aberration curves, astigmatic field curves, and an opticaldistortion curve of the optical image capturing system in the order fromleft to right according to the fourth embodiment of the presentapplication, FIG. 4C is a characteristic diagram of modulation transferof a visible light according to the fourth embodiment of the presentapplication, and FIG. 4D is a characteristic diagram of modulationtransfer of infrared rays according to the fourth embodiment of thepresent application. As shown in FIG. 4A, in order from an object sideto an image side, the optical image capturing system includes anaperture stop 400, a first lens element 410, a second lens element 420,a third lens element 430, a fourth lens element 440, a fifth lenselement 450, a sixth lens element 460, an IR-bandstop filter 480, animage plane 490, and an image sensing device 492.

The first lens element 410 has positive refractive power and it is madeof plastic material. The first lens element 410 has a convex object-sidesurface 412 and a convex image-side surface 414, and both of theobject-side surface 412 and the image-side surface 414 are aspheric. Theobject-side surface 412 has one inflection point.

The second lens element 420 has negative refractive power and it is madeof plastic material. The second lens element 420 has a convexobject-side surface 422 and a concave image-side surface 424, and bothof the object-side surface 422 and the image-side surface 424 areaspheric. The object-side surface 422 has one inflection point and theimage-side surface 424 has two inflection points.

The third lens element 430 has positive refractive power and it is madeof plastic material. The third lens element 430 has a convex object-sidesurface 432 and a convex image-side surface 434, and both of theobject-side surface 432 and the image-side surface 434 are aspheric. Theobject-side surface 432 has three inflection points and the image-sidesurface 434 has two inflection points.

The fourth lens element 440 has positive refractive power and it is madeof plastic material. The fourth lens element 440 has a concaveobject-side surface 442 and a convex image-side surface 444, and both ofthe object-side surface 442 and the image-side surface 444 are aspheric.The object-side surface 442 has two inflection points and the image-sidesurface 444 has one inflection point.

The fifth lens element 450 has positive refractive power and it is madeof plastic material. The fifth lens element 450 has a convex object-sidesurface 452 and a convex image-side surface 454, and both of theobject-side surface 452 and the image-side surface 454 are aspheric. Theobject-side surface 452 has three inflection points and the image-sidesurface 454 has two inflection points.

The sixth lens element 460 has negative refractive power and it is madeof plastic material. The sixth lens element 460 has a convex object-sidesurface 462 and a concave image-side surface 464. The object-sidesurface 462 and the image-side surface 464 both have one inflectionpoint. Hereby, the back focal length is reduced to miniaturize the lenselement effectively. In addition, the angle of incident with incominglight from an off-axis view field can be suppressed effectively and theaberration in the off-axis view field can be corrected further.

The IR-bandstop filter 480 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 460 and the image plane 490.

In the optical image capturing system of the fourth embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relation is satisfied: ΣPP=25.142 mm andf1/ΣPP=0.332. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the fourth embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relation is satisfied: ΣNP=−14.534 mm andf2/ΣNP=0.878. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 7 and Table 8.

The detailed data of the optical image capturing system of the fourthembodiment is as shown in Table 7.

TABLE 7 Data of the optical image capturing system f = 3.940 mm; f/HEP =1.8 ; HAF = 45 deg Focal Surface# Curvature Radius Thickness MaterialIndex Abbe # length 0 Object Plano At infinity 1 Ape. Stop Plano 0.000 2Lens 1 5.268187817 0.694 Plastic 1.544 55.96 8.335 3 −31.98141678 0.0004 1E+18 0.177 5 Lens 2 4.600818207 0.325 Plastic 1.642 22.46 −12.760 62.873320313 0.247 7 Lens 3 7.545434815 0.842 Plastic 1.544 55.96 9.814 8−17.78998541 0.352 9 Lens 4 −2.345566694 0.846 Plastic 1.544 55.96 2.89610 −1.065308966 0.050 11 Lens 5 11.85883661 0.375 Plastic 1.642 22.464.097 12 −3.375695316 0.050 13 Lens 6 9.192718927 0.400 Plastic 1.64222.46 −1.774 14 1.003757009 0.767 15 IR−bandstop Plano 0.420 BK_7 1.51764.13 filter 16 Plano 0.930 17 Image plane Plano 0.000 Referencewavelength (d-line) = 555 nm, shield position: clear aperture (CA) ofthe fourth plano = 1.320 mm;As for the parameters of the aspheric surfaces of the fourth embodiment,reference is made to Table 8.

TABLE 8 Aspheric Coefficients Surface # 2 3 5 6 7 8 9 k −2.976912E+01−9.000000E+01 −5.632599E+01 −6.775330E+00 −1.355488E+01 −6.847853E+01−1.452500E+00 A4   2.571998E−02 −6.591886E−02 −3.974732E−02−5.805278E−02 −3.886677E−02 −4.826957E−02 −3.964479E−02 A6  1.860553E−02   9.145645E−02   3.854546E−03   6.393928E−02−1.268655E−02 −2.043528E−03   4.292578E−02 A8 −3.488367E−01−2.178678E−01 −6.140982E−02 −1.022650E−01   4.112553E−02 −7.532372E−03−8.949003E−02 A10   1.069098E+00   2.637743E−01   4.087389E−02  8.780849E−02 −5.496756E−02   1.771374E−03   8.271459E−02 A12−1.652708E+00 −1.861199E−01   6.436621E−03 −4.487610E−02   3.038767E−02  1.376129E−03 −3.333039E−02 A14   1.397485E+00   6.895518E−02−2.144297E−02   1.185438E−02 −7.249228E−03 −4.141862E−04   6.210657E−03A16 −6.173167E−01 −1.062283E−02   6.495295E−03 −1.209823E−03  6.292737E−04   2.152106E−05 −4.423370E−04 A18   1.112092E−01  0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00   0.000000E+00 A20   0.000000E+00   0.000000E+00  0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00 Surface # 10 11 12 13 14 k −1.715384E+00 −1.096525E+01−7.387733E+01 −8.727492E+01 −4.325706E+00 A4 −1.008729E−02 −1.508345E−01−6.205870E−02   1.073801E−01 −1.726324E−03 A6   3.436981E−02  1.691599E−01   1.211279E−01 −6.600122E−02 −7.518685E−03 A8−6.725802E−02 −7.936728E−02 −6.068590E−02   1.917932E−02   2.101320E−03A10   5.078297E−02   2.003074E−02   1.491912E−02 −3.139029E−03−2.682324E−04 A12 −1.725228E−02 −3.011150E−03 −2.021807E−03  2.955909E−04   1.650810E−05 A14   2.725816E−03   2.539701E−04  1.451725E−04 −1.488823E−05 −3.391227E−07 A16 −1.625048E−04−9.623503E−06 −4.324871E−06   3.076089E−07 −4.747157E−09 A18  0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00 A20   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00   0.000000E+00

The presentation of the aspheric surface formula in the fourthembodiment is similar to that in the first embodiment. Besides thedefinitions of parameters in following tables are equal to those in thefirst embodiment so the repetitious details will not be given here.

The following contents may be deduced from Table 7 and Table 8.

Fourth embodiment (Primary reference wavelength: 555 nm) ETP1 ETP2 ETP3ETP4 ETP5 ETP6 0.501 0.458 0.716 0.643 0.309 0.633 ETP1/TP1 ETP2/TP2ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 0.721 1.410 0.850 0.760 0.823 1.582ETL EBL EIN EIR PIR EIN/ETL 6.386 1.759 4.627 0.409 0.767 0.725 SETP/EINEIR/PIR SETP STP SETP/STP BL 0.704 0.533 3.259 3.482 0.936 2.117 ED12ED23 ED34 ED45 ED56 EBL/BL 0.262 0.146 0.174 0.546 0.240 0.8309 SED SINSED/SIN ED12/ED23 ED23/ED34 ED34/ED45 1.368 0.876 1.562 1.796 0.8360.319 ED12/IN12 ED23/IN23 ED34/IN34 ED45/IN45 ED56/IN56 ED45/ED56 1.4810.591 0.495 10.919 4.799 2.275 | f/f1 | | f/f2 | | f/f3 | | f/f4 | |f/f5 | | f/f6 | 0.47268 0.30876 0.40143 1.36017 0.96159 2.22088 Σ PPR ΣNPR Σ PPR/| Σ NPR | IN12/f IN56/f TP4/(IN34 + TP4 + IN45) 3.195872.52964 1.26337 0.04485 0.01269 0.67774 | f1/f2 | | f2/f3 | (TP1 +IN12)/TP2 (TP6 + IN56)/TP5 0.65322 1.30014 2.67971 1.20000 HOS InTLHOS/HOI InS/HOS ODT % TDT % 6.47499 4.35788 1.61875 1.00000 1.602160.78956 HVT51 HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS 1.681 0.980552.90631 2.48626 0.62157 0.38398 TP2/TP3 TP3/TP4 InRS61 InRS62 | InRS61|/TP6 | InRS62 |/TP6 0.38607 0.99475 0.41602 0.53010 1.04006 1.32524MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.9 0.87 0.8 0.77 0.68 0.54 MTFI0MTFI3 MTFI7 0.67 0.55 0.55

The following contents may be deduced from Table 7 and Table 8.

Related inflection point values of second embodiment (Primary referencewavelength: 555 nm) HIF111 0.8305 HIF111/HOI 0.2076 SGI111 0.0611 |SGI111 | /( | SGI111 | +TP1) 0.0809 HIF211 0.4509 HIF211/HOI 0.1127SGI211 0.0180 | SGI211 | /( | SGI211 | +TP2) 0.0526 HIF221 0.6861HIF221/HOI 0.1715 SGI221 0.0665 | SGI221 | /( | SGI221 | +TP2) 0.1698HIF222 1.5524 HIF222/HOI 0.3881 SGI222 −0.0072 | SGI222 | /( | SGI222 |+TP2) 0.0217 HIF311 0.5043 HIF311/HOI 0.1261 SGI311 0.0140 | SGI311 | /(| SGI311 | +TP3) 0.0164 HIF312 1.3942 HIF312/HOI 0.3486 SGI312 −0.0536 |SGI312 | /( | SGI312 | +TP3) 0.0599 HIF313 1.7235 HIF313/HOI 0.4309SGI313 −0.1167 | SGI313 | /( | SGI313 | +TP3) 0.1218 HIF321 1.5285HIF321/HOI 0.3821 SGI321 −0.3642 | SGI321 | /( | SGI321 | +TP3) 0.3020HIF322 1.7113 HIF322/HOI 0.4278 SGI322 −0.4908 | SGI322 | /( | SGI322 |+TP3) 0.3683 HIF411 1.1659 HIF411/HOI 0.2915 SGI411 −0.3313 | SGI411 |/( | SGI411 | +TP4) 0.2814 HIF412 1.8790 HIF412/HOI 0.4698 SGI412−0.6038 | SGI412 | /( | SGI412 | +TP4) 0.4164 HIF421 1.2531 HIF421/HOI0.3133 SGI421 −0.6278 | SGI421 | /( | SGI421 | +TP4) 0.4259 HIF5110.2328 HIF511/HOI 0.0582 SGI511 0.0019 | SGI511 | /( | SGI511 | +TP5)0.0050 HIF512 0.7178 HIF512/HOI 0.1794 SGI512 −0.0003 | SGI512 | /( |SGI512 | +TP5) 0.0008 HIF513 1.4077 HIF513/HOI 0.3519 SGI513 0.0389 |SGI513 | /( | SGI513 | +TP5) 0.0940 HIF521 0.5852 HIF521/HOI 0.1463SGI521 −0.0396 | SGI521 | /( | SGI521 | +TP5) 0.0955 HIF522 1.5613HIF522/HOI 0.3903 SGI522 0.0294 | SGI522 | /( | SGI522 | +TP5) 0.0727HIF611 1.1874 HIF611/HOI 0.2969 SGI611 0.1488 | SGI611 | /( | SGI611 |+TP6) 0.2712 HIF621 0.9424 HIF621/HOI 0.2356 SGI621 0.2912 | SGI621 | /(| SGI621 | +TP6) 0.4213

The Fifth Embodiment (Embodiment 5)

Please refer to FIG. 5A, FIG. 5B, FIGS. 5C, and 5D. FIG. 5A is aschematic view of the optical image capturing system according to thefifths embodiment of the present application, FIG. 5B is longitudinalspherical aberration curves, astigmatic field curves, and an opticaldistortion curve of the optical image capturing system in the order fromleft to right according to the fifth embodiment of the presentapplication, FIG. 5C is a characteristic diagram of modulation transferof a visible light according to the fifth embodiment of the presentapplication and FIG. 5D is a characteristic diagram of modulationtransfer of infrared rays according to the fifth embodiment of thepresent application. As shown in FIG. 5A, in order from an object sideto an image side, the optical image capturing system includes anaperture stop 500, a first lens element 510, a second lens element 520,a third lens element 530, a fourth lens element 540, a fifth lenselement 550, a sixth lens element 560, an IR-bandstop filter 580, animage plane 590, and an Image sensing device 592.

The first lens element 510 has positive refractive power and it is madeof plastic material. The first lens element 510 has a convex object-sidesurface 512 and a convex image-side surface 514, and both of theobject-side surface 512 and the image-side surface 514 are aspheric. Theobject-side surface 512 has one inflection point.

The second lens element 520 has negative refractive power and it is madeof plastic material. The second lens element 520 has a convexobject-side surface 522 and a concave image-side surface 524, and bothof the object-side surface 522 and the image-side surface 524 areaspheric and have one inflection point.

The third lens element 530 has negative refractive power and it is madeof plastic material. The third lens element 530 has a convex object-sidesurface 532 and a concave image-side surface 534, and both of theobject-side surface 532 and the image-side surface 534 are aspheric andhave two inflection points.

The fourth lens element 540 has positive refractive power and it is madeof plastic material. The fourth lens element 540 has a convexobject-side surface 542 and a convex image-side surface 544, and both ofthe object-side surface 542 and the image-side surface 544 are aspheric.The object-side surface 542 has one inflection point and the image-sidesurface 544 has two inflection points.

The fifth lens element 550 has positive refractive power and it is madeof plastic material. The fifth lens element 550 has a concaveobject-side surface 552 and a convex image-side surface 554, and both ofthe object-side surface 552 and the image-side surface 554 are aspheric.The object-side surface 552 has two inflection points and the image-sidesurface 554 has one inflection point.

The sixth lens element 560 has negative refractive power and it is madeof plastic material. The sixth lens element 560 has a convex object-sidesurface 562 and a concave image-side surface 564. The object-sidesurface 562 and the image-side surface 564 both have one inflectionpoint. Hereby, the back focal length is reduced to miniaturize the lenselement effectively. In addition, the angle of incident with incominglight from an off-axis view field can be suppressed effectively and theaberration in the off-axis view field can be corrected further.

The IR-bandstop filter 580 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 560 and the image plane 590.

In the optical image capturing system of the fifth embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relation is satisfied: ΣPP=17.146 mm andf1/ΣPP=0.508. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the fifth embodiment, sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relation is satisfied: ΣNP=−33.920 mm andf2/ΣNP=0.625. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 9 and Table 10.

The detailed data of the optical image capturing system of the fifthembodiment is as shown in Table 9.

TABLE 9 Data of the optical image capturing system f = 4.707 mm; f/HEP =1.6 ; HAF = 40.001 deg Focal Surface# Curvature Radius ThicknessMaterial Index Abbe # length 0 Object Plano At infinity 1 Ape. StopPlano 0.000 2 Lens 1 7.855838957 0.800 Plastic 1.544 55.96 8.705 3−11.61581333 0.000 4 1E+18 0.075 5 Lens 2 4.260491116 0.325 Plastic1.584 29.88 −21.194 6 3.084627113 0.494 7 Lens 3 5.359626372 0.325Plastic 1.642 22.46 −7.898 8 2.554763888 0.116 9 Lens 4 2.9535478950.845 Plastic 1.544 55.96 4.675 10 −16.95896892 0.350 11 Lens 5−2.611639694 1.531 Plastic 1.544 55.96 3.766 12 −1.388955716 0.050 13Lens 6 2.866755728 0.923 Plastic 1.642 22.46 −4.829 14 1.306378913 0.90615 IR-bandstop Plano 0.269 BK_7 1.517 64.13 filter 16 Plano 1.081 17Image plane Plano 0.000 Reference wavelength (d-line) = 555 nm, shieldposition: clear aperture (CA) of the fourth plano = 1.520 mm;As for the parameters of the aspheric surfaces of the fifth embodiment,reference is made to Table 10.

TABLE 10 Aspheric Coefficients Surface # 2 3 5 6 7 8 9 k −7.769008E+01−2.294206E+01 −8.998595E+01 −5.254363E+01   3.012059E+00 −1.474340E+00−3.077811E+00 A4   1.663951E−02   8.752681E−02   2.281024E−01  2.004239E−01 −5.819287E−02 −9.162777E−02 −4.358891E−02 A6−9.609908E−03 −2.031369E−01 −3.856682E−01 −2.946639E−01   3.723602E−02  6.242696E−02   3.664333E−02 A8 −2.641415E−03   2.121885E−01  3.526392E−01   2.445790E−01 −5.766727E−02 −5.017373E−02 −2.315980E−02A10   6.180458E−03 −1.343413E−01 −2.012232E−01 −1.343813E−01  4.241138E−02   2.542794E−02   9.244855E−03 A12 −4.196430E−03  5.084074E−02   6.888647E−02   4.576307E−02 −1.802699E−02 −7.513155E−03−2.186457E−03 A14   1.344448E−03 −1.061141E−02 −1.272821E−02−8.730773E−03   3.947455E−03   1.170586E−03   2.668437E−04 A16−1.787890E−04   9.316844E−04   9.332312E−04   7.003246E−04 −3.328407E−04−7.327687E−05 −1.283050E−05 A18   0.000000E+00   0.000000E+00  0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00 A20   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00 Surface # 1011 12 13 14 k −2.997759E+01 −1.699552E+00 −4.432222E+00 −5.486023E−01−4.576987E+00 A4 −7.214742E−03   1.168022E−02 −6.741678E−02−2.869136E−02   1.491198E−03 A6   1.250568E−02   5.524252E−03  3.851271E−02   3.231687E−03 −3.675809E−03 A8 −9.337641E−03−7.489727E−03 −1.709735E−02 −1.114200E−03   8.906586E−04 A10  4.117993E−03   4.488701E−03   4.932851E−03   2.869713E−04−1.214585E−04 A12 −9.684850E−04 −1.164451E−03 −8.217596E−04−4.327970E−05   9.503187E−06 A14   1.116607E−04   1.385786E−04  7.399863E−05   3.339807E−06 −3.956757E−07 A16 −5.119732E−06−6.301366E−06 −2.799431E−06 −1.003529E−07   6.852189E−09 A18  0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00 A20   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00   0.000000E+00

The presentation of the aspheric surface formula in the fifth embodimentis similar to that in the first embodiment. Besides the definitions ofparameters in following tables are equal to those in the firstembodiment so the repetitious details will not be given here.

The following contents may be deduced from Table 9 and Table 10.

The following contents may be deduced from Table 9 and Table 10.

Related inflection point values of fifth embodiment (Primary referencewavelength: 555 nm) HIF111 1.0116 HIF111/HOI 0.2529 SGI111 0.0597 |SGI111 | /( | SGI111 | +TP1) 0.0694 HIF211 0.8062 HIF211/HOI 0.2016SGI211 0.0847 | SGI211 | /( | SGI211 | +TP2) 0.2068 HIF221 0.8530HIF221/HOI 0.2132 SGI221 0.1128 | SGI221 | /( | SGI221 | +TP2) 0.2577HIF311 0.5934 HIF311/HOI 0.1484 SGI311 0.0270 | SGI311 | /( | SGI311 |+TP3) 0.0767 HIF312 1.6824 HIF312/HOI 0.4206 SGI312 −0.2167 | SGI312 |/( | SGI312 | +TP3) 0.4000 HIF321 0.7793 HIF321/HOI 0.1948 SGI321 0.0927| SGI321 | /( | SGI321 | +TP3) 0.2219 HIF322 1.8789 HIF322/HOI 0.4697SGI322 0.0941 | SGI322 | /( | SGI322 | +TP3) 0.2245 HIF411 1.3393HIF411/HOI 0.3348 SGI411 0.2216 | SGI411 | /( | SGI411 | +TP4) 0.2078HIF421 1.1507 HIF421/HOI 0.2877 SGI421 −0.0378 | SGI421 | /( | SGI421 |+TP4) 0.0429 HIF422 1.7628 HIF422/HOI 0.4407 SGI422 −0.0614 | SGI422 |/( | SGI422 | +TP4) 0.0677 HIF511 1.2266 HIF511/HOI 0.3066 SGI511−0.2475 | SGI511 | /( | SGI511 | +TP5) 0.1392 HIF512 2.3169 HIF512/HOI0.5792 SGI512 −0.3432 | SGI512 | /( | SGI512 | +TP5) 0.1832 HIF5211.7174 HIF521/HOI 0.4294 SGI521 −0.8113 | SGI521 | /( | SGI521 | +TP5)0.3464 HIF611 1.1889 HIF611/HOI 0.2972 SGI611 0.2002 | SGI611 | /( |SGI611 | +TP6) 0.1782 HIF621 1.2031 HIF621/HOI 0.3008 SGI621 0.3635 |SGI621 | /( | SGI621 | +TP6) 0.2826

The Sixth Embodiment (Embodiment 6)

Please refer to FIG. 6A, FIG. 6B, FIGS. 6C, and 6D. FIG. 6A is aschematic view of the optical image capturing system according to thesixth Embodiment of the present application, FIG. 6B is longitudinalspherical aberration curves, astigmatic field curves, and an opticaldistortion curve of the optical image capturing system in the order fromleft to right according to the sixth Embodiment of the presentapplication, FIG. 6C is a characteristic diagram of modulation transferof a visible light according to the sixth embodiment of the presentapplication and FIG. 6D is a characteristic diagram of modulationtransfer of infrared rays according to the sixth embodiment of thepresent application. As shown in FIG. 6A, in order from an object sideto an image side, the optical image capturing system includes anaperture stop 600, a first lens element 610, a second lens element 620,a third lens element 630, a fourth lens element 640, a fifth lenselement 650, a sixth lens element 660, an IR-bandstop filter 680, animage plane 690, and an image sensing device 692.

The first lens element 610 has positive refractive power and it is madeof plastic material. The first lens element 610 has a convex object-sidesurface 612 and a concave image-side surface 614, and both of theobject-side surface 612 and the image-side surface 614 are aspheric andhave one inflection point.

The second lens element 620 has negative refractive power and it is madeof plastic material. The second lens element 620 has a convexobject-side surface 622 and a concave image-side surface 624, and bothof the object-side surface 622 and the image-side surface 624 areaspheric and have one inflection point.

The third lens element 630 has negative refractive power and it is madeof plastic material. The third lens element 630 has a convex object-sidesurface 632 and a concave image-side surface 634, and both of theobject-side surface 632 and the image-side surface 634 are aspheric andhave two inflection points.

The fourth lens element 640 has positive refractive power and it is madeof plastic material. The fourth lens element 640 has a convexobject-side surface 642 and a convex image-side surface 644, and both ofthe object-side surface 642 and the image-side surface 644 are aspheric.The object-side surface 642 has two inflection points and the image-sidesurface 644 has one inflection point.

The fifth lens element 650 has positive refractive power and it is madeof plastic material. The fifth lens element 650 has a concaveobject-side surface 652 and a convex image-side surface 654, and both ofthe object-side surface 652 and the image-side surface 654 are asphericand have two inflection points.

The sixth lens element 660 has negative refractive power and it is madeof plastic material. The sixth lens element 660 has a convex object-sidesurface 662 and a concave image-side surface 664. The object-sidesurface 662 and the image-side surface 664 both have one inflectionpoint. Hereby, the back focal length is reduced to miniaturize the lenselement effectively. In addition, the angle of incident with incominglight from an off-axis view field can be suppressed effectively and theaberration in the off-axis view field can be corrected further.

The IR-bandstop filter 680 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 660 and the image plane 690.

In the optical image capturing system of the sixth Embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relations are satisfied: ΣPP=16.963 mm andf1/ΣPP=0.443. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the sixth Embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relations are satisfied: ΣNP=−29.144 mm andf2/ΣNP=0.457. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 11 and Table 12.

The detailed data of the optical image capturing system of the sixthEmbodiment is as shown in Table 11.

TABLE 11 Data of the optical image capturing system f = 4.713 mm; f/HEP= 1.7; HAF = 40.000 deg Focal Surface# Curvature Radius ThicknessMaterial Index Abbe # length 0 Object Plano At infinity 1 Ape. StopPlano 0.000 2 Lens 1 3.909739014 0.694 Plastic 1.544 55.96 7.520 375.86990514 0.000 4 1E+18 0.075 5 Lens 2 6.131804368 0.325 Plastic 1.58429.88 −13.305 6 3.368669815 0.373 7 Lens 3 3.626294858 0.325 Plastic1.642 22.46 −9.951 8 2.238777773 0.134 9 Lens 4 2.873247165 0.850Plastic 1.544 55.96 4.157 10 −9.699818102 0.493 11 Lens 5 −1.7112752850.977 Plastic 1.544 55.96 5.285 12 −1.291070246 0.050 13 Lens 62.789177322 0.925 Plastic 1.642 22.46 −5.889 14 1.400897429 0.729 15IR-bandstop Plano 0.269 BK_7 1.517 64.13 filter 16 Plano 1.081 17 Imageplane Plano 0.000 Reference wavelength (d-line) = 555 nm, shieldposition: clear aperture (CA) of the fourth plano = 1.560 mm;As for the parameters of the aspheric surfaces of the sixth Embodiment,reference is made to Table 12.

TABLE 12 Aspheric Coefficients Surface # 2 3 5 6 7 8 9 k −7.769994E+01−2.294206E+01 −9.000000E+01 −5.253990E+01   1.945177E+00 −1.566477E+00−3.945608E+00 A4   1.337743E−01   3.723703E−02   1.392474E−01  2.082464E−01 −6.827014E−02 −1.195002E−01 −4.405342E−02 A6−2.192680E−01 −1.965532E−01 −3.333182E−01 −3.320451E−01   5.908127E−02  1.176086E−01   4.943602E−02 A8   2.517290E−01   2.363838E−01  3.436517E−01   3.061150E−01 −8.965738E−02 −1.141600E−01 −3.695327E−02A10 −1.986390E−01 −1.573076E−01 −1.929823E−01 −1.733317E−01  6.926778E−02   6.946864E−02   1.601537E−02 A12   9.693028E−02  6.135687E−02   6.096643E−02   5.918826E−02 −2.938715E−02 −2.467856E−02−3.767724E−03 A14 −2.635284E−02 −1.345582E−02 −1.013267E−02−1.145770E−02   6.165369E−03   4.596713E−03   3.670239E−04 A16  3.016905E−03   1.283905E−03   6.661149E−04   9.568130E−04−4.885752E−04 −3.404033E−04 −4.046246E−06 A18   0.000000E+00  0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00   0.000000E+00 A20   0.000000E+00   0.000000E+00  0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00 Surface # 10 11 12 13 14 k   9.466769E+00 −1.999109E+00−4.438010E+00 −6.925868E−01 −5.347100E+00 A4 −2.842747E−03  1.167439E−02 −1.000000E−01 −3.778601E−02 −2.638376E−03 A6  1.098178E−02   2.687348E−03   7.673034E−02   3.941447E−03−2.923733E−03 A8 −7.367216E−03 −1.096093E−02 −4.286239E−02 −7.947524E−04  8.435767E−04 A10   1.423210E−03   9.060729E−03   1.540010E−02  1.973190E−04 −1.301442E−04 A12   4.192753E−04 −2.779300E−03−3.024889E−03 −3.647095E−05   1.127261E−05 A14 −2.075023E−04  3.767371E−04   2.992338E−04   3.659907E−06 −5.112300E−07 A16  2.224316E−05 −1.927200E−05 −1.181199E−05 −1.464784E−07   9.536448E−09A18   0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00 A20   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00   0.000000E+00

In the sixth Embodiment, the presentation of the aspheric surfaceformula is similar to that in the first embodiment. Besides, thedefinitions of parameters in following tables are equal to those in thefirst embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 11 and Table 12.

Sixth embodiment (Primary reference wavelength: 555 nm) ETP1 ETP2 ETP3ETP4 ETP5 ETP6 0.404 0.473 0.441 0.514 0.832 1.087 ETP1/TP1 ETP2/TP2ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 0.582 1.456 1.358 0.605 0.852 1.175ETL EBL EIN EIR PIR EIN/ETL 7.127 1.684 5.443 0.334 0.729 0.764 SETP/EINEIR/PIR SETP STP SETP/STP BL 0.689 0.458 3.753 4.096 0.916 2.079 ED12ED23 ED34 ED45 ED56 EBL/BL 0.277 0.228 0.170 0.140 0.875 0.8100 SED SINSED/SIN ED12/ED23 ED23/ED34 ED34/ED45 1.690 1.125 1.502 1.216 1.3391.211 ED12/IN12 ED23/IN23 ED34/IN34 ED45/IN45 ED56/IN56 ED45/ED56 3.6920.610 1.269 0.285 17.499 0.161 | f/f1 | | f/f2 | | f/f3 | | f/f4 | |f/f5 | | f/f6 | 0.62675 0.35425 0.47367 1.13383 0.89178 0.80042 Σ PPR ΣNPR Σ PPR/| Σ NPR | IN12/f IN56/f TP4/(IN34 + TP4 + IN45) 2.652351.62834 1.62887 0.01591 0.01061 0.57552 | f1/f2 | | f2/f3 | (TP1 +IN12)/TP2 (TP6 + IN56)/TP5 0.56522 1.33710 2.36601 0.99869 HOS InTLHOS/HOI InS/HOS ODT % TDT % 7.30000 5.22108 1.82500 1.00000 1.607210.82978 HVT51 HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS 1.87399 0 1.946672.58687 0.64672 0.35437 TP2/TP3 TP3/TP4 InRS61 InRS62 | InRS61 |/TP6 |InRS62 |/TP6 1.00000 0.38236 0.09917 0.54946 0.10718 0.59381 MTFE0 MTFE3MTFE7 MTFQ0 MTFQ3 MTFQ7 0.92 0.88 0.8 0.82 0.68 0.52 MTFI0 MTFI3 MTFI70.56 0.64 0.27

The following contents may be deduced from Table 11 and Table 12.

Related inflection point values of sixth embodiment (Primary referencewavelength: 555 nm) HIF111 0.9869 HIF111/HOI 0.2467 SGI111 0.1127 |SGI111 | /( | SGI111 | +TP1) 0.1397 HIF121 0.3523 HIF121/HOI 0.0881SGI121 0.0011 | SGI121 | /( | SGI121 | +TP1) 0.0015 HIF211 0.6224HIF211/HOI 0.1556 SGI211 0.0343 | SGI211 | /( | SGI211 | +TP2) 0.0954HIF221 1.0806 HIF221/HOI 0.2702 SGI221 0.1663 | SGI221 | /( | SGI221 |+TP2) 0.3385 HIF311 0.7311 HIF311/HOI 0.1828 SGI311 0.0607 | SGI311 | /(| SGI311 | +TP3) 0.1573 HIF312 1.6519 HIF312/HOI 0.4130 SGI312 −0.0243 |SGI312 | /( | SGI312 | +TP3) 0.0695 HIF321 0.8083 HIF321/HOI 0.2021SGI321 0.1109 | SGI321 | /( | SGI321 | +TP3) 0.2544 HIF322 1.6598HIF322/HOI 0.4149 SGI322 0.1917 | SGI322 | /( | SGI322 | +TP3) 0.3710HIF411 1.2353 HIF411/HOI 0.3088 SGI411 0.2014 | SGI411 | /( | SGI411 |+TP4) 0.1916 HIF412 1.8961 HIF412/HOI 0.4740 SGI412 0.2724 | SGI412 | /(| SGI412 | +TP4) 0.2427 HIF421 1.9696 HIF421/HOI 0.4924 SGI421 −0.2214 |SGI421 | /( | SGI421 | +TP4) 0.2067 HIF511 1.1989 HIF511/HOI 0.2997SGI511 −0.3574 | SGI511 | /( | SGI511 | +TP5) 0.2679 HIF512 2.1466HIF512/HOI 0.5367 SGI512 −0.5464 | SGI512 | /( | SGI512 | +TP5) 0.3588HIF521 1.3877 HIF521/HOI 0.3469 SGI521 −0.5935 | SGI521 | /( | SGI521 |+TP5) 0.3780 HIF522 2.1665 HIF522/HOI 0.5416 SGI522 −0.9497 | SGI522 |/( | SGI522 | +TP5) 0.4930 HIF611 1.0267 HIF611/HOI 0.2567 SGI611 0.1528| SGI611 | /( | SGI611 | +TP6) 0.1418 HIF621 1.0921 HIF621/HOI 0.2730SGI621 0.2854 | SGI621 | /( | SGI621 | +TP6) 0.2358

The Seventh Embodiment (Embodiment 7)

Please refer to FIG. 7A and FIG. 7B, FIGS. 7C, and 7D. FIG. 7A is aschematic view of the optical image capturing system according to theseventh Embodiment of the present application, FIG. 7B is longitudinalspherical aberration curves, astigmatic field curves, and an opticaldistortion curve of the optical image capturing system in the order fromleft to right according to the seventh Embodiment of the presentapplication, FIG. 7C is a characteristic diagram of modulation transferof a visible light according to the seventh embodiment of the presentapplication and FIG. 7D is a characteristic diagram of modulationtransfer of infrared rays according to the seventh embodiment of thepresent application. As shown in FIG. 7A, in order from an object sideto an image side, the optical image capturing system includes anaperture stop 700, a first lens element 710, a second lens element 720,a third lens element 730, a fourth lens element 740, a fifth lenselement 750, a sixth lens element 760, an IR-bandstop filter 780, animage plane 790, and an image sensing device 792.

The first lens element 710 has positive refractive power and it is madeof plastic material. The first lens element 710 has a convex object-sidesurface 712 and a concave image-side surface 714, and both of theobject-side surface 712 and the image-side surface 714 are aspheric. Theobject-side surface 712 has one inflection point and the image-sidesurface 714 has two inflection points.

The second lens element 720 has negative refractive power and it is madeof plastic material. The second lens element 720 has a convexobject-side surface 722 and a concave image-side surface 724, and bothof the object-side surface 722 and the image-side surface 724 areaspheric and have two inflection points.

The third lens element 730 has negative refractive power and it is madeof plastic material. The third lens element 730 has a convex object-sidesurface 732 and a concave image-side surface 734, and both of theobject-side surface 732 and the image-side surface 734 are aspheric. Theobject-side surface 732 has two inflection points and the image-sidesurface 734 has three inflection points.

The fourth lens element 740 has positive refractive power and it is madeof plastic material. The fourth lens element 740 has a convexobject-side surface 742 and a convex image-side surface 744, and both ofthe object-side surface 742 and the image-side surface 744 are aspheric.The object-side surface 742 has one inflection point and the image-sidesurface 744 has three inflection points.

The fifth lens element 750 has positive refractive power and it is madeof plastic material. The fifth lens element 750 has a concaveobject-side surface 752 and a convex image-side surface 754, and both ofthe object-side surface 752 and the image-side surface 754 are asphericand have two inflection points.

The sixth lens element 760 has negative refractive power and it is madeof plastic material. The sixth lens element 760 has a convex object-sidesurface 762 and a concave image-side surface 764. The object-sidesurface 762 and the image-side surface 764 both have one inflectionpoint. Hereby, the back focal length is reduced to miniaturize the lenselement effectively. In addition, the angle of incident with incominglight from an off-axis view field can be suppressed effectively and theaberration in the off-axis view field can be corrected further.

The IR-bandstop filter 780 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 760 and the image plane 790.

In the optical image capturing system of the seventh Embodiment, a sumof focal lengths of all lens elements with positive refractive power isΣPP. The following relations are satisfied: ΣPP=19.912 mm andf1/ΣPP=0.383. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the seventh Embodiment, a sumof focal lengths of all lens elements with negative refractive power isΣNP. The following relations are satisfied: ΣNP=−37.245 mm andf2/ΣNP=0.364. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 13 and Table 14.

The detailed data of the optical image capturing system of the seventhEmbodiment is as shown in Table 13.

TABLE 13 Data of the optical image capturing system f = 4.722 mm ; f/HEP= 1.8; HAF = 40 deg Focal Surface # Curvature Radius Thickness MaterialIndex Abbe # length 0 Object Plano At infinity 1 Ape. Stop Plano −0.0962 Lens 1 4.017674667 0.684 Plastic 1.544 55.96 7.629 3 105.0134021 0.0004 1E+18 0.075 5 Lens 2 5.154186129 0.325 Plastic 1.584 29.88 −13.547 63.055110739 0.383 7 Lens 3 3.394319238 0.325 Plastic 1.642 22.46 −15.6748 2.447998808 0.178 9 Lens 4 4.645521898 0.900 Plastic 1.544 55.96 4.62910 −5.169619101 0.526 11 Lens 5 −1.497430088 0.800 Plastic 1.544 55.967.654 12 −1.310743543 0.050 13 Lens 6 2.646738083 0.987 Plastic 1.64222.46 -8.024 14 1.496470015 0.718 15 IR-bandstop Plano 0.269 BK_7 1.51764.13 filter 16 Plano 1.081 17 Image plane Plano 0.000 Referencewavelength (d-line) = 555 nmAs for the parameters of the aspheric surfaces of the seventhEmbodiment, reference is made to Table 14.

TABLE 14 Aspheric Coefficients Surface # 2 3 5 6 7 8 9 k −7.769994E+01−2.287814E+01 −8.999338E+01 −3.357762E+01   3.733783E−01 −1.440074E+00−1.966488E+00 A4   1.342682E−01 −1.980568E−02   7.223733E−02  1.343910E−01 −7.350535E−02 −7.575536E−02 −1.623838E−02 A6−2.484947E−01 −8.287559E−02 −2.143573E−01 −2.198588E−01   2.770471E−02  3.428303E−02   1.748199E−02 A8   3.365242E−01   1.413447E−01  2.688429E−01   2.191102E−01 −5.363556E−02 −3.520011E−02 −1.378722E−02A10 −3.113953E−01 −1.235782E−01 −1.909993E−01 −1.385503E−01  5.168318E−02   2.442048E−02   6.358563E−03 A12   1.771036E−01  6.202710E−02   7.839576E−02   5.212437E−02 −2.568195E−02 −9.755910E−03−1.797669E−03 A14 −5.573642E−02 −1.736428E−02 −1.751426E−02−1.097530E−02   6.071212E−03   2.036429E−03   2.524793E−04 A16  7.366575E−03   2.095390E−03   1.650571E−03   9.886715E−04−5.331500E−04 −1.685336E−04 −1.383999E−05 A18   1.112092E−01  0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00   0.000000E+00 A20   0.000000E+00   0.000000E+00  0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00 Surface # 10 11 12 13 14 k   3.888052E+00 −1.700265E+00−4.270645E+00 −8.903394E−01 −4.942191E+00 A4 −2.470081E−02 −1.500200E−02−1.189252E−01 −4.478355E−02 −8.591029E−03 A6   2.378759E−02  1.333168E−02   8.568416E−02   7.896640E−03   8.209777E−05 A8−1.537821E−02 −1.324404E−02 −4.476646E−02 −1.845727E−03   2.894899E−05A10   7.608495E−03   9.989938E−03   1.583555E−02   3.067580E−04−3.233196E−06 A12 −1.983705E−03 −3.081518E−03 −3.183602E−03−2.894905E−05   2.305132E−07 A14   2.357026E−04   4.244035E−04  3.292609E−04   1.143121E−06 −2.332634E−08 A16 −9.080767E−06−2.218635E−05 −1.377558E−05 −1.525635E−09   1.201183E−09 A18  0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00 A20   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00   0.000000E+00

In the seventh Embodiment, the presentation of the aspheric surfaceformula is similar to that in the first embodiment. Besides, thedefinitions of parameters in following tables are equal to those in thefirst embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 13 and Table 14.

The following contents may be deduced from Table 13 and Table 14.

Related inflection point values of seventh embodiment (Primary referencewavelength: 555 nm) HIF111 0.9957 HIF111/HOI 0.2489 SGI111 0.1121 |SGI111 | /( | SGI111 | +TP1) 0.1408 HIF121 0.1760 HIF121/HOI 0.0440SGI121 0.0001 | SGI121 | /( | SGI121 | +TP1) 0.0002 HIF122 1.4739HIF122/HOI 0.3685 SGI122 −0.1699 | SGI122 | /( | SGI122 | +TP1) 0.1990HIF211 0.6128 HIF211/HOI 0.1532 SGI211 0.0321 | SGI211 | /( | SGI211 |+TP2) 0.0898 HIF212 1.5866 HIF212/HOI 0.3967 SGI212 0.0381 | SGI212 | /(| SGI212 | +TP2) 0.1050 HIF221 0.9755 HIF221/HOI 0.2439 SGI221 0.1366 |SGI221 | /( | SGI221 | +TP2) 0.2959 HIF222 1.7172 HIF222/HOI 0.4293SGI222 0.0723 | SGI222 | /( | SGI222 | +TP2) 0.1819 HIF311 0.6259HIF311/HOI 0.1565 SGI311 0.0479 | SGI311 | /( | SGI311 | +TP3) 0.1285HIF312 1.6396 HIF312/HOI 0.4099 SGI312 −0.0911 | SGI312 | /( | SGI312 |+TP3) 0.2189 HIF321 0.7565 HIF321/HOI 0.1891 SGI321 0.0947 | SGI321 | /(| SGI321 | +TP3) 0.2257 HIF322 1.6669 HIF322/HOI 0.4167 SGI322 0.1537 |SGI322 | /( | SGI322 | +TP3) 0.3211 HIF323 1.8602 HIF323/HOI 0.4651SGI323 0.1335 | SGI323 | /( | SGI323 | +TP3) 0.2912 HIF411 1.2719HIF411/HOI 0.3180 SGI411 0.1531 | SGI411 | /( | SGI411 | +TP4) 0.1454HIF421 1.3751 HIF421/HOI 0.3438 SGI421 −0.2142 | SGI421 | /( | SGI421 |+TP4) 0.1923 HIF422 1.7199 HIF422/HOI 0.4300 SGI422 −0.3109 | SGI422 |/( | SGI422 | +TP4) 0.2568 HIF423 1.8918 HIF423/HOI 0.4729 SGI423−0.3578 | SGI423 | /( | SGI423 | +TP4) 0.2845 HIF511 1.2235 HIF511/HOI0.3059 SGI511 −0.4605 | SGI511 | /( | SGI511 | +TP5) 0.3652 HIF5122.1266 HIF512/HOI 0.5317 SGI512 −0.7231 | SGI512 | /( | SGI512 | +TP5)0.4747 HIF521 1.3841 HIF521/HOI 0.3460 SGI521 −0.6202 | SGI521 | /( |SGI521 | +TP5) 0.4366 HIF522 2.1523 HIF522/HOI 0.5381 SGI522 −1.0323 |SGI522 | /( | SGI522 | +TP5) 0.5633 HIF611 1.0129 HIF611/HOI 0.2532SGI611 0.1543 | SGI611 | /( | SGI611 | +TP6) 0.1351 HIF621 1.1044HIF621/HOI 0.2761 SGI621 0.2813 | SGI621 | /( | SGI621 | +TP6) 0.2217

The Eight Embodiment (Embodiment 8)

Please refer to FIG. 8A, FIG. 8B, FIGS. 8C, and 8D. FIG. 8A is aschematic view of the optical image capturing system according to theeighth Embodiment of the present application, FIG. 8B is longitudinalspherical aberration curves, astigmatic field curves, and an opticaldistortion curve of the optical image capturing system in the order fromleft to right according to the eighth Embodiment of the presentapplication, FIG. 8C is a characteristic diagram of modulation transferof a visible light according to the eighth embodiment of the presentapplication and FIG. 8D is a characteristic diagram of modulationtransfer of infrared rays according to the eighth embodiment of thepresent application. As shown in FIG. 8A, in order from an object sideto an image side, the optical image capturing system includes anaperture stop 800, a first lens element 810, a second lens element 820,a third lens element 830, a fourth lens element 840, a fifth lenselement 850, a sixth lens element 860, an IR-bandstop filter 880, animage plane 890, and an image sensing device 892.

The first lens element 810 has positive refractive power and it is madeof plastic material. The first lens element 810 has a convex object-sidesurface 812 and a concave image-side surface 814, and both of theobject-side surface 812 and the image-side surface 814 are aspheric andhave one inflection point.

The second lens element 820 has negative refractive power and it is madeof plastic material. The second lens element 820 has a concaveobject-side surface 822 and a convex image-side surface 824, and both ofthe object-side surface 822 and the image-side surface 824 are aspheric.The object-side surface 822 has one inflection point.

The third lens element 830 has negative refractive power and it is madeof plastic material. The third lens element 830 has a convex object-sidesurface 832 and a concave image-side surface 834, and both of theobject-side surface 832 and the image-side surface 834 are aspheric andhave two inflection points.

The fourth lens element 840 has positive refractive power and it is madeof plastic material. The fourth lens element 840 has a convexobject-side surface 842 and a concave image-side surface 844, and bothof the object-side surface 842 and the image-side surface 844 areaspheric and have one inflection point.

The fifth lens element 850 has positive refractive power and it is madeof plastic material. The fifth lens element 850 has a concaveobject-side surface 852 and a convex image-side surface 854, and both ofthe object-side surface 852 and the image-side surface 854 are asphericand have two inflection points.

The sixth lens element 860 has negative refractive power and it is madeof plastic material. The sixth lens element 860 has a convex object-sidesurface 862 and a concave image-side surface 864. The object-sidesurface 862 has one inflection point and the image-side surface 864 hastwo inflection points. Hereby, the back focal length is reduced tominiaturize the lens element effectively. In addition, the angle ofincident with incoming light from an off-axis view field can besuppressed effectively and the aberration in the off-axis view field canbe corrected further.

The IR-bandstop filter 880 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 860 and the image plane 890.

In the optical image capturing system of the eighth Embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relations are satisfied: ΣPP=17.538 mm andf1/ΣPP=0.341. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the eighth Embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relations are satisfied: ΣNP=−46.654 mm andf2/ΣNP=0.182. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 15 and Table 16.

The detailed data of the optical image capturing system of the eighthEmbodiment is as shown in Table 15.

TABLE 15 Data of the optical image capturing system f = 5.667 mm ; f/HEP= 1.9; HAF = 35 deg Focal Surface# Curvature Radius Thickness MaterialIndex Abbe # length 0 Object Plano At infinity 1 Ape. Stop Plano −0.3652 Lens 1 2.591880817 0.845 Plastic 1.544 55.96 5.986 3 11.05720635 0.0004 1E+18 0.513 5 Lens 2 −4.381758749 0.325 Plastic 1.642 22.46 −8.473 6−22.38377039 0.230 7 Lens 3 2.908343516 0.325 Plastic 1.642 22.46−34.179 8 2.457683673 0.088 9 Lens 4 2.868547627 0.831 Plastic 1.54455.96 6.037 10 19.78870206 0.485 11 Lens 5 −4.194458806 0.963 Plastic1.636 23.89 5.515 12 −2.088985307 0.140 13 Lens 6 6.786054081 0.935Plastic 1.642 22.46 −4.002 14 1.77395462 0.371 15 IR-bandstop Plano0.269 BK_7 1.517 64.13 filter 16 Plano 1.081 17 Image plane Plano 0.000Reference wavelength (d-line) = 555 nmAs for the parameters of the aspheric surfaces of the eighth Embodiment,reference is made to Table 16.

TABLE 16 Aspheric Coefficients Surface # 2 3 5 6 7 8 9 k −4.250043E+00−1.140000E+01 −2.312391E+00 −1.318308E+01   4.857524E−01 −2.552440E+00−7.852248E+00 A4   2.919507E−02 −1.120451E−02   8.216037E−04−1.964981E−03 −3.526899E−02 −6.507124E−02 −4.947003E−02 A6 −7.660275E−03−5.061038E−03 −2.983621E−02 −5.268312E−02 −4.381936E−02   2.096577E−02  2.221682E−02 A8   3.878660E−03   5.099624E−03   5.239919E−02  8.340364E−02   3.343078E−02 −1.950739E−02 −9.547535E−04 A10−2.177592E−03 −5.176256E−03 −4.298628E−02 −6.362338E−02 −2.402621E−02  5.685915E−03 −4.109296E−03 A12   5.585560E−04   2.743840E−03  1.993328E−02   2.758541E−02   1.056077E−02   3.190679E−04  2.095722E−03 A14 −3.060913E−05 −8.109357E−04 −5.001144E−03−6.554065E−03 −2.738716E−03 −5.270405E−04 −4.910795E−04 A16−2.093070E−05   9.448891E−05   5.210720E−04   6.453541E−04  3.320981E−04   9.949121E−05   4.485559E−05 A18   2.758492E−02  0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00   0.000000E+00 A20   0.000000E+00   0.000000E+00  0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00 Surface # 10 11 12 13 14 k   2.650002E−01   2.655216E+00−1.205439E+01 −9.580774E−01 −3.510269E+00 A4 −6.238639E−03  5.701781E−02 −4.417265E−02 −2.496909E−02 −6.965547E−02 A6−2.383625E−02 −6.028441E−02 −1.326982E−02 −9.102789E−02   1.986360E−02A8   8.907805E−03   1.486966E−02   1.353832E−02   7.319411E−02−3.501119E−03 A10   4.362158E−03   5.469440E−03 −4.169430E−03−2.763540E−02   3.500147E−04 A12 −3.483493E−03 −3.450703E−03  7.867468E−04   5.775219E−03 −1.702447E−05 A14   7.744739E−04  6.548178E−04 −8.829804E−05 −6.446209E−04   9.779107E−08 A16−5.944149E−05 −4.416567E−05   3.993121E−06   2.981003E−05   1.565012E−08A18   0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00 A20   0.000000E+00   0.000000E+00   0.000000E+00  0.000000E+00   0.000000E+00

In the eighth Embodiment, the presentation of the aspheric surfaceformula is similar to that in the first embodiment. Besides, thedefinitions of parameters in following tables are equal to those in thefirst embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 15 and Table 16.

Eighth embodiment (Primary reference wavelength: 555 nm) ETP1 ETP2 ETP3ETP4 ETP5 ETP6 0.409 0.474 0.401 0.611 0.772 1.341 ETP1/TP1 ETP2/TP2ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 0.484 1.458 1.232 0.736 0.802 1.435ETL EBL EIN EIR PIR EIN/ETL 6.965 1.445 5.520 0.095 0.371 0.793 SETP/EINEIR/PIR SETP STP SETP/STP BL 0.726 0.256 4.008 4.224 0.949 1.721 ED12ED23 ED34 ED45 ED56 EBL/BL 0.266 0.352 0.178 0.222 0.494 0.8396 SED SINSED/SIN ED12/ED23 ED23/ED34 ED34/ED45 1.512 1.456 1.039 0.756 1.9740.805 ED12/IN12 ED23/IN23 ED34/IN34 ED45/IN45 ED56/IN56 ED45/ED56 0.5191.532 2.033 0.457 3.520 0.449 | f/f1 | | f/f2| | f/f3 | | f/f4 | | f/f5| | f/f6 | 0.94671 0.66888 0.16581 0.93881 1.02761 1.41612 Σ PPR Σ NPR ΣPPR/| Σ NPR | IN12/f IN56/f TP4/(IN34 + TP4 + IN45) 2.91313 2.250801.29426 0.09048 0.02475 0.59199 | f1/f2 | | f2/f3 | (TP1 + IN12)/TP2(TP6 + IN56)/TP5 0.70652 0.24789 4.17785 1.11612 HOS InTL HOS/HOIInS/HOS ODT % TDT % 7.40000 5.67923 1.85000 0.95071 1.61414 1.0759 HVT51HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS 0 0 0.74702 1.84649 0.461620.24953 TP2/TP3 TP3/TP4 InRS61 InRS62 | InRS61 |/TP6 | InRS62 |/TP61.00000 0.39117 −0.85655 −0.19654 0.91645 0.21028 MTFE0 MTFE3 MTFE7MTFQ0 MTFQ3 MTFQ7 0.93 0.85 0.82 0.8 0.66 0.56 MTFI0 MTFI3 MTFI7 0.5 0.8 0.33

The following contents may be deduced from Table 15 and Table 16.

Related inflection point values of eighth Embodiment (Primary referencewavelength: 555 nm) HIF111 1.3870 HIF111/HOI 0.3467 SGI111 0.3813 |SGI111 | /( | SGI111 | +TP1) 0.3109 HIF121 0.6930 HIF121/HOI 0.1733SGI121 0.0185 | SGI121 | /( | SGI121 | +TP1) 0.0215 HIF211 1.5770HIF211/HOI 0.3943 SGI211 −0.2756 | SGI211 | /( | SGI211 | +TP2) 0.4589HIF311 0.6993 HIF311/HOI 0.1748 SGI311 0.0738 | SGI311 | /( | SGI311 |+TP3) 0.1850 HIF312 1.5978 HIF312/HOI 0.3994 SGI312 −0.0533 | SGI312 |/( | SGI312 | +TP3) 0.1410 HIF321 0.7084 HIF321/HOI 0.1771 SGI321 0.0842| SGI321 | /( | SGI321 | +TP3) 0.2058 HIF322 1.5620 HIF322/HOI 0.3905SGI322 0.0747 | SGI322 | /( | SGI322 | +TP3) 0.1869 HIF411 0.9204HIF411/HOI 0.2301 SGI411 0.1044 | SGI411 | /( | SGI411 | +TP4) 0.1117HIF421 0.4877 HIF421/HOI 0.1219 SGI421 0.0054 | SGI421 | /( | SGI421 |+TP4) 0.0064 HIF511 1.5183 HIF511/HOI 0.3796 SGI511 −0.3053 | SGI511 |/( | SGI511 | +TP5) 0.2407 HIF512 1.8133 HIF512/HOI 0.4533 SGI512−0.4312 | SGI512 | /( | SGI512 | +TP5) 0.3093 HIF521 1.5152 HIF521/HOI0.3788 SGI521 −0.4990 | SGI521 | /( | SGI521 | +TP5) 0.3413 HIF5222.0231 HIF522/HOI 0.5058 SGI522 −0.7736 | SGI522 | /( | SGI522 | +TP5)0.4455 HIF611 0.4554 HIF611/HOI 0.1139 SGI611 0.0135 | SGI611 | /( |SGI611 | +TP6) 0.0143 HIF621 0.7610 HIF621/HOI 0.1902 SGI621 0.1279 |SGI621 | /( | SGI621 | +TP6) 0.1204 HIF622 3.1046 HIF622/HOI 0.7762SGI622 −0.1373 | SGI622 | /( | SGI622 | +TP6) 0.1281

The above-mentioned descriptions represent merely the exemplaryembodiment of the present disclosure, without any intention to limit thescope of the present disclosure thereto. Various equivalent changes,alternations or modifications based on the claims of present disclosureare all consequently viewed as being embraced by the scope of thepresent disclosure.

What is claimed is:
 1. An optical image capturing system, from an objectside to an image side, comprising: a first lens element with refractivepower; a second lens element with refractive power; a third lens elementwith refractive power; a fourth lens element with refractive power; afifth lens element with refractive power; a sixth lens element withrefractive power; and an image plane; wherein the optical imagecapturing system consists of six lens elements with refractive power, amaximum height for image formation on the image plane perpendicular tothe optical axis in the optical image capturing system is denoted byHOI, at least two lens elements among the first through sixth lenselements have at least one inflection point on at least one surfacethereof, at least one lens element among the first through sixth lenselements has positive refractive power, focal lengths of the firstthrough sixth lens elements are f1, f2, f3, f4, f5 and f6 respectively,a focal length of the optical image capturing system is f, an entrancepupil diameter of the optical image capturing system is HEP, a distanceon an optical axis from an axial point on an object-side surface of thefirst lens element to an axial point on the image plane is HOS, a halfof a maximum view angle of the optical image capturing system is HAF,thicknesses in parallel with an optical axis of the first through sixthlens elements at height ½ HEP respectively are ETP1, ETP2, ETP3, ETP4,ETP5 and ETP6, a sum of ETP1 to ETP6 described above is SETP,thicknesses of the first through sixth lens elements on the optical axisrespectively are TP1, TP2, TP3, TP4, TP5 and TP6, a sum of TP1 to TP6described above is STP, and the following relations are satisfied:1.0≦f/HEP≦10.0, 0 deg<HAF≦150 deg and 0.5≦SETP/STP<1.
 2. The opticalimage capturing system of claim 1, wherein a horizontal distance inparallel with the optical axis from a coordinate point on theobject-side surface of the first lens element at height ½ HEP to theimage plane is ETL, a horizontal distance in parallel with the opticalaxis from a coordinate point on the object-side surface of the firstlens element at height ½ HEP to a coordinate point on the image-sidesurface of the sixth lens element at height ½ HEP is EIN, and thefollowing relation is satisfied: 0.2≦EIN/ETL<1.
 3. The optical imagecapturing system of claim 2, wherein the thicknesses in parallel withthe optical axis of the first through sixth lens elements at height ½HEP respectively are ETP1, ETP2, ETP3, ETP4, ETP5 and ETP6, the sum ofETP1 to ETP6 described above is SETP, and the following relation issatisfied: 0.3≦SETP/EIN<1.
 4. The optical image capturing system ofclaim 1, wherein the optical image capturing system comprises a lightfiltration element, the light filtration element is located between thesixth lens element and the image plane, a distance in parallel with theoptical axis from a coordinate point on the image-side surface of thesixth lens element at height ½ HEP to the light filtration element isEIR, a distance in parallel with the optical axis from an axial point onthe image-side surface of the sixth lens element to the light filtrationelement is PIR, and the following relation is satisfied:0.1≦EIR/PIR≦1.1.
 5. The optical image capturing system of claim 1,wherein a thickness of the fourth lens element on the optical axis isTP4, a thickness of the fifth lens element on the optical axis is TP5, athickness of the sixth lens element on the optical axis is TP6, and thefollowing relations are satisfied: TP4≧TP5 and TP4≧TP6.
 6. The opticalimage capturing system of claim 1, wherein contrast transfer rates ofmodulation transfer with space frequencies of 55 cycles/mm (MTF values)of a visible light at the optical axis on the image plane, 0.3 HOI and0.7 HOI are respectively denoted by MTFE0, MTFE3 and MTFE7, and thefollowing relations are satisfied: MTFE0≧0.2, MTFE3≧0.01 and MTFE7≧0.01.7. The optical image capturing system of claim 1, wherein a half ofmaximum view angle of the optical image capturing system is HAF, and thefollowing relation is satisfied: 0 deg<|HAF≦100 deg.
 8. The opticalimage capturing system of claim 1, wherein a horizontal distance inparallel with the optical axis from a coordinate point on the image-sidesurface of the sixth lens element at height ½ HEP to the image plane isEBL, a horizontal distance in parallel with the optical axis from anaxial point on the image-side surface of the sixth lens element to theimage plane is BL, and the following relation is satisfied:0.1≦EBL/BL<1.1.
 9. The optical image capturing system of claim 1,further comprising an aperture stop, a distance from the aperture stopto the image plane on the optical axis is InS, an image sensing deviceis disposed on the image plane, and the following relations aresatisfied: 0.1≦InS/HOS≦1.1 and 0≦HIF/HOI≦0.9.
 10. An optical imagecapturing system, from an object side to an image side, comprising: afirst lens element with refractive power; a second lens element withrefractive power; a third lens element with refractive power; a fourthlens element with refractive power; a fifth lens element with refractivepower; a sixth lens element with refractive power; and an image plane;wherein the optical image capturing system consists of six lens elementswith refractive power, a maximum height for image formation on the imageplane perpendicular to the optical axis in the optical image capturingsystem is denoted by HOI, at least two lens elements among the firstthrough sixth lens element have at least one inflection point on atleast one surface thereof, at least one lens element among the firstthrough third lens elements has positive refractive power, at least onelens element among the fourth through sixth lens elements has positiverefractive power, focal lengths of the first through sixth lens elementsare f1, f2, f3, f4, f5 and f6 respectively, a focal length of theoptical image capturing system is f, an entrance pupil diameter of theoptical image capturing system is HEP, a distance on an optical axisfrom an axial point on an object-side surface of the first lens elementto an axial point on the image plane is HOS, a half of a maximum viewangle of the optical image capturing system is HAF, a horizontaldistance in parallel with the optical axis from a coordinate point onthe object-side surface of the first lens element at height ½ HEP to theimage plane is ETL, a horizontal distance in parallel with the opticalaxis from a coordinate point on the object-side surface of the firstlens element at height ½ HEP to a coordinate point on the image-sidesurface of the sixth lens element at height ½ HEP is EIN, and thefollowing relations are satisfied: 1.0≦f/HEP≦10.0, 0 deg<HAF≦150 deg and0.2≦EIN/ETL<1.
 11. The optical image capturing system of claim 10,wherein a horizontal distance in parallel with the optical axis from acoordinate point on the image-side surface of the fifth lens element atheight ½ HEP to a coordinate point on the object-side surface of thesixth lens element at height ½ HEP is ED56, a distance from the fifthlens element to the sixth lens element on the optical axis is IN56, andthe following relation is satisfied: 0<ED56/IN56≦50.
 12. The opticalimage capturing system of claim 10, wherein a horizontal distance inparallel with the optical axis from a coordinate point on the image-sidesurface of the first lens element at height ½ HEP to a coordinate pointon the object-side surface of the second lens element at height ½ HEP isED12, a distance from the first lens element to the second lens elementon the optical axis is IN12, and the following relation is satisfied:0<ED12/IN12<10.
 13. The optical image capturing system of claim 10,wherein a thickness in parallel with the optical axis of the second lenselement at height ½ HEP is ETP2, a thickness of the second lens elementon the optical axis is TP2, and the following relation is satisfied:0<ETP2/TP2≦3.
 14. The optical image capturing system of claim 10,wherein a thickness in parallel with the optical axis of the fifth lenselement at height ½ HEP is ETP5, a thickness of the fifth lens elementon the optical axis is TP5, and the following relation is satisfied:0<ETP5/TP5≦3.
 15. The optical image capturing system of claim 10,wherein a thickness in parallel with the optical axis of the sixth lenselement at height ½ HEP is ETP6, a thickness of the sixth lens elementon the optical axis is TP6, and the following relation is satisfied:0<ETP6/TP6≦5.
 16. The optical image capturing system of claim 10,wherein a distance from the first lens element to the second lenselement on the optical axis is IN12, and the following relation issatisfied: 0<IN12/f≦60.
 17. The optical image capturing system of claim10, wherein contrast transfer rates of modulation transfer with spatialfrequencies of 55 cycles/mm of an infrared operation wavelength 850 nmat the optical axis on the image plane, 0.3 HOI and 0.7 HOI arerespectively denoted by MTFI0, MTFI3 and MTFI7, and the followingrelations are satisfied: MTFI0≧0.01, MTFI3≧0.01 and MTFI7≧0.01.
 18. Theoptical image capturing system of claim 10, wherein contrast transferrates of modulation transfer with space frequencies of 110 cycles/mm ofa visible light at the optical axis on the image plane, 0.3 HOI and 0.7HOI are respectively denoted by MTFQ0, MTFQ3 and MTFQ7, and thefollowing relations are satisfied: MTFQ0≧0.2, MTFQ3≧0.01 and MTFQ7≧0.01.19. The optical image capturing system of claim 10, wherein at least oneof the first, the second, the third, the fourth, the fifth and the sixthlens elements is a light filtration element with a wavelength of lessthan 500 nm.
 20. An optical image capturing system, from an object sideto an image side, comprising: a first lens element with positiverefractive power; a second lens element with refractive power; a thirdlens element with refractive power; a fourth lens element withrefractive power; a fifth lens element with refractive power; a sixthlens element with refractive power, and an image plane; wherein theoptical image capturing system consists of six lens elements withrefractive power and at least three lens elements of the six lenselements are made of glass material, a maximum height for imageformation on the image plane perpendicular to the optical axis in theoptical image capturing system is denoted by HOI, and at least one lenselement among the second through sixth lens elements has positiverefractive power, at least three lens elements among the first throughsixth lens elements respectively have at least one inflection point onat least one surface thereof, and focal lengths of the first throughsixth lens elements are f1, f2, f3, f4, f5 and f6 respectively, a focallength of the optical image capturing system is f, an entrance pupildiameter of the optical image capturing system is HEP, a half of maximumview angle of the optical image capturing system is HAF, a distance onan optical axis from an axial point on an object-side surface of thefirst lens element to an axial point on the image plane is HOS, ahorizontal distance in parallel with the optical axis from a coordinatepoint on the object-side surface of the first lens element at height ½HEP to the image plane is ETL, a horizontal distance in parallel withthe optical axis from a coordinate point on the object-side surface ofthe first lens element at height ½ HEP to a coordinate point on theimage-side surface of the sixth lens element at height ½ HEP is EIN, andthe following relations are satisfied: 1.0≦f/HEP≦3.5, 0 deg<HAF≦150 degand 0.2≦EIN/ETL<1.
 21. The optical image capturing system of claim 20,wherein a horizontal distance in parallel with the optical axis from acoordinate point on the image-side surface of the sixth lens element atheight ½ HEP to the image plane is EBL, a horizontal distance inparallel with the optical axis from an axial point on the image-sidesurface of the sixth lens element to the image plane is BL, and thefollowing relation is satisfied: 0.1≦EBL/BL≦1.1.
 22. The optical imagecapturing system of claim 20, wherein a distance from the fourth lenselement to the fifth lens element on the optical axis is IN45, adistance from the fifth lens element to the sixth lens element on theoptical axis is IN56, a horizontal distance in parallel with the opticalaxis from a coordinate point on the image-side surface of the fourthlens element at height ½ HEP to a coordinate point on the object-sidesurface of the fifth lens element at height ½ HEP is ED45, a horizontaldistance in parallel with the optical axis from a coordinate point onthe image-side surface of the fifth lens element at height ½ HEP to acoordinate point on the object-side surface of the sixth lens element atheight ½ HEP is ED56, a thickness in parallel with the optical axis ofthe fourth lens element at height ½ HEP is ETP4, a thickness in parallelwith the optical axis of the fifth lens element at height ½ HEP is ETP5,a thickness in parallel with the optical axis of the sixth lens elementat height ½ HEP is ETP6, a thickness of the fourth lens element on theoptical axis is TP4, a thickness of the fifth lens element on theoptical axis is TP5, a thickness of the sixth lens element on theoptical axis is TP6, and the following relation is satisfied:(ETP4+ED45+ETP5+ED56+ETP6)>(TP4+IN45+TP5+IN56+TP6).
 23. The opticalimage capturing system of claim 20, wherein a distance from the fifthlens element to the sixth lens element on the optical axis is IN56, andthe following relation is satisfied: 0<IN56/f≦5.0.
 24. The optical imagecapturing system of claim 20, wherein a thickness of the fourth lenselement on the optical axis is TP4, a thickness of the fifth lenselement on the optical axis is TP5, a thickness of the sixth lenselement on the optical axis is TP6, and the following relation issatisfied: TP4≧TP6 or TP5≧TP6.
 25. The optical image capturing system ofclaim 20, further comprising an aperture stop, an image sensing deviceand a driving module, the image sensing device is disposed on the imageplane, a distance from the aperture stop to the image plane on theoptical axis is InS, the driving module and the six lens elements coupleto each other and shifts are produced for the six lens elements, and thefollowing relation is satisfied: 0.1≦InS/HOS≦1.1.